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TRANSCRIPT
European Journal of Scientific Research
ISSN 1450-216X Vol22 No4 (2008) pp584-601
copy EuroJournals Publishing Inc 2008
httpwwweurojournalscomejsrhtm
On Heuristic Viewpoints Concerning the Mass Energy and Light
Concepts in Quantum Physics
Bahjat R J Muhyedeen
Department of Chemistry College of Science
University of Baghdad Jadriyah Baghdad Iraq
Contact e-mail nucleardatagmailcom
Abstract
The concept of conversion of mass to energy is discussed in chemical and nuclear
reactions to show it is incorrect The annihilation reactions of electron-positron are
discussed to be disintegration processes A primitive nuclear model is suggested to focus on
three main points the outer shells of the nucleus called electromagnetic belt the inner
nuclear shells called sphere nuclear shell model and the magnetons The magnetons and
conservons are the main components of the protons and neutrons The nuclear fusion
reactions are discussed and showed they have to pass the fifth state of matter called nuclear
transparency then finally reach the sixth state of matter called nuclear magma (finally
collected as black hole) The quantization of light by Planck is argued to be of wave-form
and not particle-form represented by photons These discrete packets of energy are called
frequentons A novel non-relativistic mass-energy equivalence is derived as E=mbc where
b is a new universal particle speed constant equal to 0603797 x 108 ms which gives
Em= 18101351214 x 1016
Jkg or 1u= 187607 MeV The ratio of mbcmc2
(187607)(93149) is equal to 02014 The Total Kinetic Energy (TKE) of fission
fragments of 235
U is found to be 3721 MeVbc rather than 1847 MeVc2 based on the
speculative E=mc2 Other non-relativistic quantum equations are deduced for high speed
charged particles such as p=mb b=λυ λ=hmb E=mvb and E=mb2
Keywords E=mc2 E=mbc Mass-Energy Equivalence photon-frequenton photon new
fifth and sixth states for matter universal particle speed constant b
1 Introduction The physical concepts of mass and energy and their relation to the universe were continually changed
throughout history by Greek Arab and Chinese philosophers However the most acceptable definitions
for mass and energy were translated into formula by Leibniz over the period 1676-1689 The mass
concept is usually related to the energy The mass is a fundamental concept in chemistry and it is a
central concept of classical mechanics and related subjects Although inertial mass (f=ma) passive
gravitational mass (f=Mg) and active gravitational mass are conceptually distinct no experiment has
ever clearly demonstrated any difference between them The concept of energy and its transformations
is extremely useful in explaining and predicting most natural phenomena Energy transformations in
the universe over time are characterized by various kinds of potential energy which has been available
since the Big Bang later being released (ie transformed to more active types of energy such as kinetic
or radiant energy) when a triggering mechanism is available During the 19th
century and 20th
century
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 585
the concepts became more realistic for both issues with a number of scientists sharing in the
crystallization of these concepts enabling a greater depth of understanding the secret of the universe
In the early 20th
century scientists started an investigation of the atom structure after the
discovery of the electron theorized by Richard Laming (1838ndash1851) and G Johnstone Stoney (1874)
and discovered by JJ Thomson (1897) the proton theorized by William Prout (1815) and discovered
by Ernest Rutherford (1919) and the neutron discovered by James Chadwick (1932) The theoretical
and experimental researches on the mass-energy atom waves and particles led to the branch of
fundamental sciences that deals with atomic and subatomic systems which we today call quantum
mechanics It is the basic mathematical framework of many fields of physics and chemistry including
condensed matter physics solid-state physics atomic physics molecular physics computational
chemistry quantum chemistry particle physics nuclear physics and chemistry quantum
chromodynamics and quantum gravity The foundations of quantum mechanics were established
during the first half of the 20th
century by Max Planck Albert Einstein Ernest Rutherford Niels Bohr
Louis de Broglie Max Born Werner Heisenberg Erwin Schroumldinger John von Neumann Paul Dirac
Wolfgang Pauli and others
The theoretical and experimental works in nuclear physics result in the formation of the
Standard Model (1970 to 1973) (Glashow 1961 Weinberg 1967 Kane 1987 Bromley 2000)
Although the Standard Model well describes the elementary particles and composite particles it is still
considered as a provisional theory rather than a truly fundamental one Many physicists find this model
to be unsatisfactory due to its many undermined parameters many fundamental particles the non-
observation of the Higgs boson and other more theoretical considerations such as the hierarchy
problem
Therefore some new speculative theories beyond the Standard Model extruded attempts to
remedy these deficiencies According to Preon Theory -coined by Jogesh Pati and Abdus Salam in
1974- (Pati and Salam 1974 Dugne et al 2002) there are one or more orders of particles more
fundamental than those found in the Standard Model called preons which are derived from pre-
quarks which look like ldquoparticle zoo modelrdquo that came before it The interest in preons has vanished
since the simplest models were experimentally ruled out in the 1980s
The Grand unification Theory attempts to combine the electroweak interaction with the strong
interaction into a single grand unified theory (GUT) (Encyclopedia Britannica 2008) GUT predicts
that at extremely high energies (above 1014 GeV) the electromagnetic weak nuclear and strong
nuclear forces are fused into a single unified field (Parker B 1993 Hawking S 1988) Such a force
would be spontaneously broken into the three forces by a Higgs-like mechanism However the non-
observation of proton decay made it less important
The Supersymmetry tried to extend the Standard Model by adding an additional class of
symmetries to the Lagrangian These symmetries exchange fermionic particles with bosonic ones In
other words in a supersymmetric theory for every type of boson there exists a corresponding type of
fermion and vice-versa Such symmetry predicts the existence of supersymmetric particles
abbreviated as sparticles which include the sleptons squarks neutralinos and charginos But these
particles are so heavy that they need more experiments to be verified (Baer and Xerxes 2006) As of
2008 there is no direct evidence that supersymmetry is a symmetry of nature (Freund 1986 Martin
1999 Lykken 1996 Drees 1996 Arygres 2001)
String Theory is an incomplete mathematical approach to theoretical physics whose building
blocks are one-dimensional extended objects called strings rather than the zero-dimensional point
particles that form the basis for the standard model of particle physics (Arygres 2001 Cooper et al
1995 Junker 1996) The string theory mainly the M-theory out of the five string theories suggest that
all particles that make up matter and energy are comprised of strings measuring at the Planck length
equals 1616252x10-35
m that exists in an 11-dimensional universe to prevent tears in the fabric of
space using the uncertainty principle whereas our own existence is merely a 4-brane inside which
exist the 3 space dimensions and the 1 time dimension that we observe (Schwartz 1998 Troost 2005
586 Bahjat R J Muhyedeen
Witten 2005) The String theory is formulated in terms of an action principle either the Nambu-Goto
action (using the principles of Lagrangian mechanics) or the Polyakov action (using conformal field
theory) which describes how strings move through space and time These strings vibrate at different
frequencies which determine mass electric charge color charge and spin A string can be open (a line)
or closed in a loop As a string moves through space it sweeps out a two-dimensional surface f(τσ)
called a world sheet One particularly interesting prediction of the string theory is the existence of
extremely massive counterparts of ordinary particles due to vibrational excitations of the fundamental
string Another important prediction is the existence of a massless spin-2 particle behaving like the
graviton The main aim of this theory is to treat the universe through the quantum mechanics and
classical mechanic
The aim of this paper is to correct some concepts on mass-energy relationship mass of
radiation nuclear processes and quantization of light and to derive a new formula for mass-energy
equivalence in addition to derive some equations for the non-relativistic elementary and composite
particles that move in speed less than the speed of light
2 The mass-energy relationship The dualism behavior of mass and energy is a very old idea since Thales of Miletus (Greek
philosopher 624 BCndashca 546 BC) then Galileo (Italian) in 1638 (Singer 1941) then in 1676
mathematically formulated by Gottfried Leibniz (German) (E=mv2 called it Vis Viva) (Leibniz
1716 Mackie 1845) and others In 1717 Isaac Newton (English) speculated that gross bodies and
light are inter-convertible into each other (Newton 1704 1727) Lavoisiers experiments in 1774
supported the law of conservation of mass in primitive manner (Arthur 1993) In the literature the
recalibration of Leibniz formula to include the coefficient of a half viz (12mv2) was mainly the
consequence of the work of Gaspard-Gustave Coriolis (called it quantity of work) and Jean-Victor
Poncelet (called it mechanical work) over the period 1819-1839
3 Are mass and energy convertible The scientists at the era from 1500 up to 1800 were focused on the stars and planets and they thought
that the energy emitted from stars is finally converted to the mass and vice versa to keep the eternity of
the universe and they also thought that when body emits radiation it will lose some of its weight These
confused ideas grew up and were well crystallized as concepts of classical mechanics from 1800-1920
These concepts were clearly shown in the works of S Tolver Preston in 1875 (E Δmc2)
(Preston1875) Jules Henri Poincaregrave in 1900 [mv=(Ec2)c] (Poincarersquo 1900) Olinto De Pretto who
speculated E=mc2
in 1903-1904 (Pretto 1904 Bartocci 1999) Fritz Hasenoumlhrl in 1904 (m= 4E3c2)
(Ohrl and Sitzungen 1904 Ohrl 1905) Einstein in 1905 (E=mc2 from speculative origin) which is
only true under special conditions (Einstein 1905) and Max Planck in 1907 [(m-M)=Ec2] (Planck
1907 1908) and Einstein also in 1909 [(m-M)=Lc2] (Einstein 1909) Frederick Soddy and M
Henri Becquerel both have predicted that the energy of radiation is at the cost of mass (Soddy 1904)
In 1900 Poincaregrave and Abraham in 1904 showed that W = mc2 can be derived for the case that
the radiation is fully absorbed by a metal plate In the duration 1900-1905 Poincareacute Kaufmann
Abraham and Hasenoumlhrl have shown that the mass of electrons increase during acceleration The
mass increase can easily be derived for this case as the energy is transferred through an
electromagnetic wave by the help of the Poyntingndashvector (Poincaregrave 1900 Kaufmann 1902 Abraham
1903 1904 Hasenoumlhrl 1904) These ideas bred out two main imprecise concepts in physics that
firstly the mass and energy are convertible secondly the radiation has mass
In our belief that the idea of mass-energy conversion is incorrect The mass and the energy are
inconvertible Since the Big Bang the energy was stored mainly in two big reservoirs
1- binding energies of the electrons in the quantized atomic orbitals of the atoms
2- binding energies of the fermions in the quantized nuclear shells of the nuclei of the atoms
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 587
We daily use these stored energies in various chemical and nuclear reactions and there is no mass
converted to energy or vice versa This energy is continuously generated at these two big reservoirs
The speculative equation E=mc2
was misinterpreted when they considered c2 as the conversion
factor from mass to energy The correct understanding is that the head c has to be multiplied with the
mass (mc) to measure the momentum of the particle while next c is considered as the conversion factor
from the momentum unit to the energy unit We will explain this concept in forthcoming paper
4 Energy from chemical reactions In the chemical reactions it is absolutely clear that there is no loss in the mass of the material in any
reaction The process is based on breaking bonds and forming new others The difference in binding
energies which are stored in the atomic orbitals will be released in the case of exothermal reactions In
the case of endothermic reactions we have to supply energy to the electrons of the reactants to help
them to undergo reaction For example the combustion of the hydrocarbon will result in H2O and CO2
5 Energy from nuclear reactions Of course the nuclear visions of nucleus structure and its components is still the greatest obstacle in
the gaining a deep understanding of how can we calculate the energy of nuclear reactions via the
nuclear binding energies like the atomic orbitals far from the mass defect concept The
experimentalists need more time of hard works in nuclear science to collect more facts about the real
structure of elementary particles (Fermions QuarksLeptons etc) and composite particles (Hadrons
Baryons Hyperons Nucleons Mesons) They have to improve the optical model which uses optical
laws in its calculation (Fernbach S et al 1949) shell model of Eugene Paul Wigner Maria
Goeppert-Mayer and J Hans D Jensen which uses the Pauli principle to describe the structure of
the nucleus in terms of energy levels (Cohen 1971 Rohlf 1994) and liquid drop model of
Weizsaumlckers formula (Freedman and Young 2004) to reach to an integrated model that combine the
shell model (quantum mechanical) and the collective models
Anyhow the quark theory is still immature to explain the nuclear transformation of the proton
and neutron in a clear way The fundamental particles that form the neutron are still not clear The
quark theory tells us that the neutron is created from three quarks (two down and one up) But the mass
of neutron is not fixed in different nuclei (supposing the proton mass is fixed due to its high stability)
For example the mass of the free neutron in atomic mass units u is (1008665 u) and the mass of
neutron in deuterium is (10062767459 u) and the mass of the neutron in tritium is (10041121177 u)
The nuclear workers said that the decrease in the nuclide mass is converted into the binding energy in
the host nucleus Now we may ask which part of quark of neutron will convert to energy to form the
binding energy when the neutron gets inside the host nucleus
6 Proposal for new nuclear model The proposed nuclear model focus on three main points the outer shell of the nucleus which might be
called the electromagnetic belt (sheath) and the inner new nuclear shell model which might be called
the sphere nuclear shells in addition to modification of the Quark Model of Gell-Mann (Georgi
Eidelman S et al 2004) The aim of the model is to set up a new nuclear model which is capable to
show that the nuclear energy calculation is based on the energy generated by the sub-quark particles
and not on converting some mass of baryons to binding energy
In the present paper we will submit the basic idea of this model and later in the upcoming paper
we will try to give a more detailed structure This crude nuclear model supposes that both the
electromagnetic belt surrounding the nucleus the inner sphere nuclear shells and the sub-quarks
play an important role in nucleus concept We may outline the basic points of this model as below
I- This nuclear model predicts that the protons neutrons and all fermions are composed of integer
multiple of the sub-quarks These sub-quarks are of high magnetic field and align strongly as magnetic
588 Bahjat R J Muhyedeen
dipoles in such a way that they build the fermion in form of N-S dipoles packages Their high magnetic
properties are responsible for the strong nuclear forces We call these magnetic sub-quarks magnetons
In addition there are new elementary particles inside the nucleus which may be called conservon that
keeps both neutron and proton to obey the conservation law and control the conservation of mass
number ∆A=0 linear momentum ∆p=0 total energy ∆E=0 charge ∆Z=0 and spins ∆I=0 during the
nuclear reactions The conservons are also responsible for keeping the mass stability of neutrons and
the proton inside the nuclei The mass of conservon is of integer multiple of the sub-quarks
magnetons mass The binding energy between the proton and the neutron occurs with help from
conservon particles The conservon particles control the nuclear processes The sub-quarks magnetons
and conservons are the main components of the protons and neutrons inside the nuclei
II- The sub-quarks magnetons are the basic building blocks of the fermions The annihilation reactions
of electron-positron are pseudo-annihilation processes The annihilation reactions break the laws of
conservations These pseudo-annihilation reactions are misinterpreted by nuclear workers These
reactions represent inelastic scattering When the electron and the positron collide their
electromagnetic fields will interfere in a deconstructive way (disintegration process) which results in
producing radiation This rule may apply to all matter and antimatter reactions
III- The model predicts that the electromagnetic belt controls the projectile and the target during the
nuclear reactions The electromagnetic belt represents the net charged electromagnetic field of the
nuclear forces of the nuclei We think that the profound understanding of the unfathomable coulomb
barrier surrounding the nucleus is very important The electromagnetic belt is also regulating the
strong nuclear force generated by the magnetons which controls the required mass of the baryon inside
the nuclei and the attraction force of the electrons in the atomic orbitals The charged nuclear forces
will create binding energy of nucleons in the nucleus The source of the binding energy is derived from
the charged nuclear forces rather than from converting some mass of hadrons during the entrance
IV- The model proposed that the protons have certain stable mass while the neutron has several stable
masses that depend on the isotope Z and N The neutron stable mass is available in the stable isotopes
V- The proposed new sphere nuclear shell model states that the nucleus is a composite of many spheres
occupied by 1-4 nucleons and these spheres are distributed among hypothetical nuclear shells It is an
independent-particle nuclear shell model to expect the decay modes and to identify the fertile and
fissile nuclide through shell configuration The sphere has to be filled in the form of (pnpn) ie the
proton first then the neutron next and so on The model explains why some isotopes emit alpha particle
The details of this model will be explained in the forthcoming paper
VI- In the core of the sun or any star this electromagnetic belt of small nuclei became less dense in a
region of high electromagnetic pressure and temperature above 10 million oK In such circumstances
the electromagnetic belt becomes loose (of very low barrier) and the protons and neutrons in their
nuclei are more free to undergo the fusion reactions in equilibrium state (or reversible nuclear
reaction) but the reaction will move toward the stable nuclei of magic numbers when these reactions
occurred at region place little far from the sun core (ie in the circumferences of the core region) which
releases high energies This phase represents a fifth state of matter beyond plasma (where the electrons
are free) in which protons and neutrons are moving more freely in their nuclei This phase is called
ldquoNuclear Transparencyrdquo which endures extra super high temperature and pressure and electromagnetic
field In such Nuclear Transparency phase there is good probability to build the more stable nuclei of
magic number in the sun core such as Fe Ni O Si S Mg C Ne Ca and Cr and even higher nuclides
(actinides) The fifth state may be responsible for the state of hydrostatic equilibrium neither
contracting nor expanding over time
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 589
VII- In the deep core of the sun and stars the nuclei become completely bare of the electromagnetic
belt and the nucleons become free of their nuclei after passing the Nuclear Transparency phase In this
region some of the fermions will be analyzed to their elementary particles the magnetic sub-quarks
magnetons which accumulated in nebulous form and might be called nuclear magma The nuclear
magma starts getting cold and dark because no heat can be absorbed or emitted due to the amorphous
structure The nuclear magma is denser than the nuclei and of high magnetic property and they bind
each other through very strong charged nuclear forces This nuclear magma will be born in the core of
the sun and it moves up toward the surface as ldquocold and darkrdquo mass so called a sunspot These
sunspots (nuclear magma) are collected together through a million of years to form a black hole state
and this nuclear magma state of matter may be called the sixth state of matter The black hole is the
source of the magnetons for creation of elements and then the compounds in the universe When the
star gets old it starts losing its gases and the plasma region will evaporate leaving the cold and
magnetic sunspot alone to form the black hole The number of sunspots in the stars is indicative of the
age of the star The end life of any star is a black hole If a big mass of hydrogen gas will strike the
black hole it will ignite it again to create a new star and so on
This phase ldquonuclear magmardquo is beyond the meta Nuclear Transparency and looks like the
results announced by CERN (European Organization for Nuclear Research) that stated they have
discovered a new state of matter in 2000 which they called quark-gluon plasma It is a phase of
quantum chromodynamics which exists at extremely high temperature andor density and consists of
(almost) free quarks and gluons which are the basic building blocks of matter We can say the CERN
quark-gluon plasma state is a transition state between Nuclear Transparency and the nuclear magma
(finally the black hole) sixth state of matter
VIII- We hope that the workers in nuclear research laboratories try to get a controlling fusion reaction
through three main settings 1- high force of electromagnetic field 2- high pressure 3- flash of high
temperature (Lasergt1018
W) via advanced inertial confinement fusion (AICF) integrated with ion
beam on Deuterium and Tritium nuclei to make their electromagnetic belt more loose in terms of
picoseconds to reach the Nuclear Transparency phase and get a controlled fusion reaction through
controlling the force of the electromagnetic field taking into consideration the Lawson criterion
(Lawson 1957) The trials should go farther than tokamaks and stellarators technology (as in
Torsatron Heliotron and Helias) The stellarator technology lacks high pressure The technologies used
in magnetic confinement fusion and inertial confinement fusion are usually using only two of the three
settings mentioned above thus lessening their efficiency But generally the magnetic field is more
important than the pressure therefore as we expect the future of magnetic confinement fusion
technology is more promising than the inertial confinement fusion The magnetic field is very
necessary to loosen the electromagnetic belts which help the nuclei get into Nuclear Transparency to
undergo fusion reactions
In conclusion the magnetons are basic building blocks of the fermions The protons and
neutrons are composed of the integer multiple of sub-quarks elementary particles magnetons The
protons have certain stable mass and the neutron have several stables masses depending on the isotope
Z and N The conservons control the conservation of mass number linear momentum total energy
charge and spins during the nuclear reactions law of conservations The nuclei in the universe have
been built in the Nuclear Transparency phase with huge binding energies saved in the nuclei and these
energies are liberated during the nuclear processes and no mass will be converted to energy The same
thing happens to nuclear fission and decay processes so no mass will convert to energy or vice versa
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
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[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
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[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
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[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
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[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
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[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
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[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
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[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
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[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 585
the concepts became more realistic for both issues with a number of scientists sharing in the
crystallization of these concepts enabling a greater depth of understanding the secret of the universe
In the early 20th
century scientists started an investigation of the atom structure after the
discovery of the electron theorized by Richard Laming (1838ndash1851) and G Johnstone Stoney (1874)
and discovered by JJ Thomson (1897) the proton theorized by William Prout (1815) and discovered
by Ernest Rutherford (1919) and the neutron discovered by James Chadwick (1932) The theoretical
and experimental researches on the mass-energy atom waves and particles led to the branch of
fundamental sciences that deals with atomic and subatomic systems which we today call quantum
mechanics It is the basic mathematical framework of many fields of physics and chemistry including
condensed matter physics solid-state physics atomic physics molecular physics computational
chemistry quantum chemistry particle physics nuclear physics and chemistry quantum
chromodynamics and quantum gravity The foundations of quantum mechanics were established
during the first half of the 20th
century by Max Planck Albert Einstein Ernest Rutherford Niels Bohr
Louis de Broglie Max Born Werner Heisenberg Erwin Schroumldinger John von Neumann Paul Dirac
Wolfgang Pauli and others
The theoretical and experimental works in nuclear physics result in the formation of the
Standard Model (1970 to 1973) (Glashow 1961 Weinberg 1967 Kane 1987 Bromley 2000)
Although the Standard Model well describes the elementary particles and composite particles it is still
considered as a provisional theory rather than a truly fundamental one Many physicists find this model
to be unsatisfactory due to its many undermined parameters many fundamental particles the non-
observation of the Higgs boson and other more theoretical considerations such as the hierarchy
problem
Therefore some new speculative theories beyond the Standard Model extruded attempts to
remedy these deficiencies According to Preon Theory -coined by Jogesh Pati and Abdus Salam in
1974- (Pati and Salam 1974 Dugne et al 2002) there are one or more orders of particles more
fundamental than those found in the Standard Model called preons which are derived from pre-
quarks which look like ldquoparticle zoo modelrdquo that came before it The interest in preons has vanished
since the simplest models were experimentally ruled out in the 1980s
The Grand unification Theory attempts to combine the electroweak interaction with the strong
interaction into a single grand unified theory (GUT) (Encyclopedia Britannica 2008) GUT predicts
that at extremely high energies (above 1014 GeV) the electromagnetic weak nuclear and strong
nuclear forces are fused into a single unified field (Parker B 1993 Hawking S 1988) Such a force
would be spontaneously broken into the three forces by a Higgs-like mechanism However the non-
observation of proton decay made it less important
The Supersymmetry tried to extend the Standard Model by adding an additional class of
symmetries to the Lagrangian These symmetries exchange fermionic particles with bosonic ones In
other words in a supersymmetric theory for every type of boson there exists a corresponding type of
fermion and vice-versa Such symmetry predicts the existence of supersymmetric particles
abbreviated as sparticles which include the sleptons squarks neutralinos and charginos But these
particles are so heavy that they need more experiments to be verified (Baer and Xerxes 2006) As of
2008 there is no direct evidence that supersymmetry is a symmetry of nature (Freund 1986 Martin
1999 Lykken 1996 Drees 1996 Arygres 2001)
String Theory is an incomplete mathematical approach to theoretical physics whose building
blocks are one-dimensional extended objects called strings rather than the zero-dimensional point
particles that form the basis for the standard model of particle physics (Arygres 2001 Cooper et al
1995 Junker 1996) The string theory mainly the M-theory out of the five string theories suggest that
all particles that make up matter and energy are comprised of strings measuring at the Planck length
equals 1616252x10-35
m that exists in an 11-dimensional universe to prevent tears in the fabric of
space using the uncertainty principle whereas our own existence is merely a 4-brane inside which
exist the 3 space dimensions and the 1 time dimension that we observe (Schwartz 1998 Troost 2005
586 Bahjat R J Muhyedeen
Witten 2005) The String theory is formulated in terms of an action principle either the Nambu-Goto
action (using the principles of Lagrangian mechanics) or the Polyakov action (using conformal field
theory) which describes how strings move through space and time These strings vibrate at different
frequencies which determine mass electric charge color charge and spin A string can be open (a line)
or closed in a loop As a string moves through space it sweeps out a two-dimensional surface f(τσ)
called a world sheet One particularly interesting prediction of the string theory is the existence of
extremely massive counterparts of ordinary particles due to vibrational excitations of the fundamental
string Another important prediction is the existence of a massless spin-2 particle behaving like the
graviton The main aim of this theory is to treat the universe through the quantum mechanics and
classical mechanic
The aim of this paper is to correct some concepts on mass-energy relationship mass of
radiation nuclear processes and quantization of light and to derive a new formula for mass-energy
equivalence in addition to derive some equations for the non-relativistic elementary and composite
particles that move in speed less than the speed of light
2 The mass-energy relationship The dualism behavior of mass and energy is a very old idea since Thales of Miletus (Greek
philosopher 624 BCndashca 546 BC) then Galileo (Italian) in 1638 (Singer 1941) then in 1676
mathematically formulated by Gottfried Leibniz (German) (E=mv2 called it Vis Viva) (Leibniz
1716 Mackie 1845) and others In 1717 Isaac Newton (English) speculated that gross bodies and
light are inter-convertible into each other (Newton 1704 1727) Lavoisiers experiments in 1774
supported the law of conservation of mass in primitive manner (Arthur 1993) In the literature the
recalibration of Leibniz formula to include the coefficient of a half viz (12mv2) was mainly the
consequence of the work of Gaspard-Gustave Coriolis (called it quantity of work) and Jean-Victor
Poncelet (called it mechanical work) over the period 1819-1839
3 Are mass and energy convertible The scientists at the era from 1500 up to 1800 were focused on the stars and planets and they thought
that the energy emitted from stars is finally converted to the mass and vice versa to keep the eternity of
the universe and they also thought that when body emits radiation it will lose some of its weight These
confused ideas grew up and were well crystallized as concepts of classical mechanics from 1800-1920
These concepts were clearly shown in the works of S Tolver Preston in 1875 (E Δmc2)
(Preston1875) Jules Henri Poincaregrave in 1900 [mv=(Ec2)c] (Poincarersquo 1900) Olinto De Pretto who
speculated E=mc2
in 1903-1904 (Pretto 1904 Bartocci 1999) Fritz Hasenoumlhrl in 1904 (m= 4E3c2)
(Ohrl and Sitzungen 1904 Ohrl 1905) Einstein in 1905 (E=mc2 from speculative origin) which is
only true under special conditions (Einstein 1905) and Max Planck in 1907 [(m-M)=Ec2] (Planck
1907 1908) and Einstein also in 1909 [(m-M)=Lc2] (Einstein 1909) Frederick Soddy and M
Henri Becquerel both have predicted that the energy of radiation is at the cost of mass (Soddy 1904)
In 1900 Poincaregrave and Abraham in 1904 showed that W = mc2 can be derived for the case that
the radiation is fully absorbed by a metal plate In the duration 1900-1905 Poincareacute Kaufmann
Abraham and Hasenoumlhrl have shown that the mass of electrons increase during acceleration The
mass increase can easily be derived for this case as the energy is transferred through an
electromagnetic wave by the help of the Poyntingndashvector (Poincaregrave 1900 Kaufmann 1902 Abraham
1903 1904 Hasenoumlhrl 1904) These ideas bred out two main imprecise concepts in physics that
firstly the mass and energy are convertible secondly the radiation has mass
In our belief that the idea of mass-energy conversion is incorrect The mass and the energy are
inconvertible Since the Big Bang the energy was stored mainly in two big reservoirs
1- binding energies of the electrons in the quantized atomic orbitals of the atoms
2- binding energies of the fermions in the quantized nuclear shells of the nuclei of the atoms
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 587
We daily use these stored energies in various chemical and nuclear reactions and there is no mass
converted to energy or vice versa This energy is continuously generated at these two big reservoirs
The speculative equation E=mc2
was misinterpreted when they considered c2 as the conversion
factor from mass to energy The correct understanding is that the head c has to be multiplied with the
mass (mc) to measure the momentum of the particle while next c is considered as the conversion factor
from the momentum unit to the energy unit We will explain this concept in forthcoming paper
4 Energy from chemical reactions In the chemical reactions it is absolutely clear that there is no loss in the mass of the material in any
reaction The process is based on breaking bonds and forming new others The difference in binding
energies which are stored in the atomic orbitals will be released in the case of exothermal reactions In
the case of endothermic reactions we have to supply energy to the electrons of the reactants to help
them to undergo reaction For example the combustion of the hydrocarbon will result in H2O and CO2
5 Energy from nuclear reactions Of course the nuclear visions of nucleus structure and its components is still the greatest obstacle in
the gaining a deep understanding of how can we calculate the energy of nuclear reactions via the
nuclear binding energies like the atomic orbitals far from the mass defect concept The
experimentalists need more time of hard works in nuclear science to collect more facts about the real
structure of elementary particles (Fermions QuarksLeptons etc) and composite particles (Hadrons
Baryons Hyperons Nucleons Mesons) They have to improve the optical model which uses optical
laws in its calculation (Fernbach S et al 1949) shell model of Eugene Paul Wigner Maria
Goeppert-Mayer and J Hans D Jensen which uses the Pauli principle to describe the structure of
the nucleus in terms of energy levels (Cohen 1971 Rohlf 1994) and liquid drop model of
Weizsaumlckers formula (Freedman and Young 2004) to reach to an integrated model that combine the
shell model (quantum mechanical) and the collective models
Anyhow the quark theory is still immature to explain the nuclear transformation of the proton
and neutron in a clear way The fundamental particles that form the neutron are still not clear The
quark theory tells us that the neutron is created from three quarks (two down and one up) But the mass
of neutron is not fixed in different nuclei (supposing the proton mass is fixed due to its high stability)
For example the mass of the free neutron in atomic mass units u is (1008665 u) and the mass of
neutron in deuterium is (10062767459 u) and the mass of the neutron in tritium is (10041121177 u)
The nuclear workers said that the decrease in the nuclide mass is converted into the binding energy in
the host nucleus Now we may ask which part of quark of neutron will convert to energy to form the
binding energy when the neutron gets inside the host nucleus
6 Proposal for new nuclear model The proposed nuclear model focus on three main points the outer shell of the nucleus which might be
called the electromagnetic belt (sheath) and the inner new nuclear shell model which might be called
the sphere nuclear shells in addition to modification of the Quark Model of Gell-Mann (Georgi
Eidelman S et al 2004) The aim of the model is to set up a new nuclear model which is capable to
show that the nuclear energy calculation is based on the energy generated by the sub-quark particles
and not on converting some mass of baryons to binding energy
In the present paper we will submit the basic idea of this model and later in the upcoming paper
we will try to give a more detailed structure This crude nuclear model supposes that both the
electromagnetic belt surrounding the nucleus the inner sphere nuclear shells and the sub-quarks
play an important role in nucleus concept We may outline the basic points of this model as below
I- This nuclear model predicts that the protons neutrons and all fermions are composed of integer
multiple of the sub-quarks These sub-quarks are of high magnetic field and align strongly as magnetic
588 Bahjat R J Muhyedeen
dipoles in such a way that they build the fermion in form of N-S dipoles packages Their high magnetic
properties are responsible for the strong nuclear forces We call these magnetic sub-quarks magnetons
In addition there are new elementary particles inside the nucleus which may be called conservon that
keeps both neutron and proton to obey the conservation law and control the conservation of mass
number ∆A=0 linear momentum ∆p=0 total energy ∆E=0 charge ∆Z=0 and spins ∆I=0 during the
nuclear reactions The conservons are also responsible for keeping the mass stability of neutrons and
the proton inside the nuclei The mass of conservon is of integer multiple of the sub-quarks
magnetons mass The binding energy between the proton and the neutron occurs with help from
conservon particles The conservon particles control the nuclear processes The sub-quarks magnetons
and conservons are the main components of the protons and neutrons inside the nuclei
II- The sub-quarks magnetons are the basic building blocks of the fermions The annihilation reactions
of electron-positron are pseudo-annihilation processes The annihilation reactions break the laws of
conservations These pseudo-annihilation reactions are misinterpreted by nuclear workers These
reactions represent inelastic scattering When the electron and the positron collide their
electromagnetic fields will interfere in a deconstructive way (disintegration process) which results in
producing radiation This rule may apply to all matter and antimatter reactions
III- The model predicts that the electromagnetic belt controls the projectile and the target during the
nuclear reactions The electromagnetic belt represents the net charged electromagnetic field of the
nuclear forces of the nuclei We think that the profound understanding of the unfathomable coulomb
barrier surrounding the nucleus is very important The electromagnetic belt is also regulating the
strong nuclear force generated by the magnetons which controls the required mass of the baryon inside
the nuclei and the attraction force of the electrons in the atomic orbitals The charged nuclear forces
will create binding energy of nucleons in the nucleus The source of the binding energy is derived from
the charged nuclear forces rather than from converting some mass of hadrons during the entrance
IV- The model proposed that the protons have certain stable mass while the neutron has several stable
masses that depend on the isotope Z and N The neutron stable mass is available in the stable isotopes
V- The proposed new sphere nuclear shell model states that the nucleus is a composite of many spheres
occupied by 1-4 nucleons and these spheres are distributed among hypothetical nuclear shells It is an
independent-particle nuclear shell model to expect the decay modes and to identify the fertile and
fissile nuclide through shell configuration The sphere has to be filled in the form of (pnpn) ie the
proton first then the neutron next and so on The model explains why some isotopes emit alpha particle
The details of this model will be explained in the forthcoming paper
VI- In the core of the sun or any star this electromagnetic belt of small nuclei became less dense in a
region of high electromagnetic pressure and temperature above 10 million oK In such circumstances
the electromagnetic belt becomes loose (of very low barrier) and the protons and neutrons in their
nuclei are more free to undergo the fusion reactions in equilibrium state (or reversible nuclear
reaction) but the reaction will move toward the stable nuclei of magic numbers when these reactions
occurred at region place little far from the sun core (ie in the circumferences of the core region) which
releases high energies This phase represents a fifth state of matter beyond plasma (where the electrons
are free) in which protons and neutrons are moving more freely in their nuclei This phase is called
ldquoNuclear Transparencyrdquo which endures extra super high temperature and pressure and electromagnetic
field In such Nuclear Transparency phase there is good probability to build the more stable nuclei of
magic number in the sun core such as Fe Ni O Si S Mg C Ne Ca and Cr and even higher nuclides
(actinides) The fifth state may be responsible for the state of hydrostatic equilibrium neither
contracting nor expanding over time
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 589
VII- In the deep core of the sun and stars the nuclei become completely bare of the electromagnetic
belt and the nucleons become free of their nuclei after passing the Nuclear Transparency phase In this
region some of the fermions will be analyzed to their elementary particles the magnetic sub-quarks
magnetons which accumulated in nebulous form and might be called nuclear magma The nuclear
magma starts getting cold and dark because no heat can be absorbed or emitted due to the amorphous
structure The nuclear magma is denser than the nuclei and of high magnetic property and they bind
each other through very strong charged nuclear forces This nuclear magma will be born in the core of
the sun and it moves up toward the surface as ldquocold and darkrdquo mass so called a sunspot These
sunspots (nuclear magma) are collected together through a million of years to form a black hole state
and this nuclear magma state of matter may be called the sixth state of matter The black hole is the
source of the magnetons for creation of elements and then the compounds in the universe When the
star gets old it starts losing its gases and the plasma region will evaporate leaving the cold and
magnetic sunspot alone to form the black hole The number of sunspots in the stars is indicative of the
age of the star The end life of any star is a black hole If a big mass of hydrogen gas will strike the
black hole it will ignite it again to create a new star and so on
This phase ldquonuclear magmardquo is beyond the meta Nuclear Transparency and looks like the
results announced by CERN (European Organization for Nuclear Research) that stated they have
discovered a new state of matter in 2000 which they called quark-gluon plasma It is a phase of
quantum chromodynamics which exists at extremely high temperature andor density and consists of
(almost) free quarks and gluons which are the basic building blocks of matter We can say the CERN
quark-gluon plasma state is a transition state between Nuclear Transparency and the nuclear magma
(finally the black hole) sixth state of matter
VIII- We hope that the workers in nuclear research laboratories try to get a controlling fusion reaction
through three main settings 1- high force of electromagnetic field 2- high pressure 3- flash of high
temperature (Lasergt1018
W) via advanced inertial confinement fusion (AICF) integrated with ion
beam on Deuterium and Tritium nuclei to make their electromagnetic belt more loose in terms of
picoseconds to reach the Nuclear Transparency phase and get a controlled fusion reaction through
controlling the force of the electromagnetic field taking into consideration the Lawson criterion
(Lawson 1957) The trials should go farther than tokamaks and stellarators technology (as in
Torsatron Heliotron and Helias) The stellarator technology lacks high pressure The technologies used
in magnetic confinement fusion and inertial confinement fusion are usually using only two of the three
settings mentioned above thus lessening their efficiency But generally the magnetic field is more
important than the pressure therefore as we expect the future of magnetic confinement fusion
technology is more promising than the inertial confinement fusion The magnetic field is very
necessary to loosen the electromagnetic belts which help the nuclei get into Nuclear Transparency to
undergo fusion reactions
In conclusion the magnetons are basic building blocks of the fermions The protons and
neutrons are composed of the integer multiple of sub-quarks elementary particles magnetons The
protons have certain stable mass and the neutron have several stables masses depending on the isotope
Z and N The conservons control the conservation of mass number linear momentum total energy
charge and spins during the nuclear reactions law of conservations The nuclei in the universe have
been built in the Nuclear Transparency phase with huge binding energies saved in the nuclei and these
energies are liberated during the nuclear processes and no mass will be converted to energy The same
thing happens to nuclear fission and decay processes so no mass will convert to energy or vice versa
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
586 Bahjat R J Muhyedeen
Witten 2005) The String theory is formulated in terms of an action principle either the Nambu-Goto
action (using the principles of Lagrangian mechanics) or the Polyakov action (using conformal field
theory) which describes how strings move through space and time These strings vibrate at different
frequencies which determine mass electric charge color charge and spin A string can be open (a line)
or closed in a loop As a string moves through space it sweeps out a two-dimensional surface f(τσ)
called a world sheet One particularly interesting prediction of the string theory is the existence of
extremely massive counterparts of ordinary particles due to vibrational excitations of the fundamental
string Another important prediction is the existence of a massless spin-2 particle behaving like the
graviton The main aim of this theory is to treat the universe through the quantum mechanics and
classical mechanic
The aim of this paper is to correct some concepts on mass-energy relationship mass of
radiation nuclear processes and quantization of light and to derive a new formula for mass-energy
equivalence in addition to derive some equations for the non-relativistic elementary and composite
particles that move in speed less than the speed of light
2 The mass-energy relationship The dualism behavior of mass and energy is a very old idea since Thales of Miletus (Greek
philosopher 624 BCndashca 546 BC) then Galileo (Italian) in 1638 (Singer 1941) then in 1676
mathematically formulated by Gottfried Leibniz (German) (E=mv2 called it Vis Viva) (Leibniz
1716 Mackie 1845) and others In 1717 Isaac Newton (English) speculated that gross bodies and
light are inter-convertible into each other (Newton 1704 1727) Lavoisiers experiments in 1774
supported the law of conservation of mass in primitive manner (Arthur 1993) In the literature the
recalibration of Leibniz formula to include the coefficient of a half viz (12mv2) was mainly the
consequence of the work of Gaspard-Gustave Coriolis (called it quantity of work) and Jean-Victor
Poncelet (called it mechanical work) over the period 1819-1839
3 Are mass and energy convertible The scientists at the era from 1500 up to 1800 were focused on the stars and planets and they thought
that the energy emitted from stars is finally converted to the mass and vice versa to keep the eternity of
the universe and they also thought that when body emits radiation it will lose some of its weight These
confused ideas grew up and were well crystallized as concepts of classical mechanics from 1800-1920
These concepts were clearly shown in the works of S Tolver Preston in 1875 (E Δmc2)
(Preston1875) Jules Henri Poincaregrave in 1900 [mv=(Ec2)c] (Poincarersquo 1900) Olinto De Pretto who
speculated E=mc2
in 1903-1904 (Pretto 1904 Bartocci 1999) Fritz Hasenoumlhrl in 1904 (m= 4E3c2)
(Ohrl and Sitzungen 1904 Ohrl 1905) Einstein in 1905 (E=mc2 from speculative origin) which is
only true under special conditions (Einstein 1905) and Max Planck in 1907 [(m-M)=Ec2] (Planck
1907 1908) and Einstein also in 1909 [(m-M)=Lc2] (Einstein 1909) Frederick Soddy and M
Henri Becquerel both have predicted that the energy of radiation is at the cost of mass (Soddy 1904)
In 1900 Poincaregrave and Abraham in 1904 showed that W = mc2 can be derived for the case that
the radiation is fully absorbed by a metal plate In the duration 1900-1905 Poincareacute Kaufmann
Abraham and Hasenoumlhrl have shown that the mass of electrons increase during acceleration The
mass increase can easily be derived for this case as the energy is transferred through an
electromagnetic wave by the help of the Poyntingndashvector (Poincaregrave 1900 Kaufmann 1902 Abraham
1903 1904 Hasenoumlhrl 1904) These ideas bred out two main imprecise concepts in physics that
firstly the mass and energy are convertible secondly the radiation has mass
In our belief that the idea of mass-energy conversion is incorrect The mass and the energy are
inconvertible Since the Big Bang the energy was stored mainly in two big reservoirs
1- binding energies of the electrons in the quantized atomic orbitals of the atoms
2- binding energies of the fermions in the quantized nuclear shells of the nuclei of the atoms
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 587
We daily use these stored energies in various chemical and nuclear reactions and there is no mass
converted to energy or vice versa This energy is continuously generated at these two big reservoirs
The speculative equation E=mc2
was misinterpreted when they considered c2 as the conversion
factor from mass to energy The correct understanding is that the head c has to be multiplied with the
mass (mc) to measure the momentum of the particle while next c is considered as the conversion factor
from the momentum unit to the energy unit We will explain this concept in forthcoming paper
4 Energy from chemical reactions In the chemical reactions it is absolutely clear that there is no loss in the mass of the material in any
reaction The process is based on breaking bonds and forming new others The difference in binding
energies which are stored in the atomic orbitals will be released in the case of exothermal reactions In
the case of endothermic reactions we have to supply energy to the electrons of the reactants to help
them to undergo reaction For example the combustion of the hydrocarbon will result in H2O and CO2
5 Energy from nuclear reactions Of course the nuclear visions of nucleus structure and its components is still the greatest obstacle in
the gaining a deep understanding of how can we calculate the energy of nuclear reactions via the
nuclear binding energies like the atomic orbitals far from the mass defect concept The
experimentalists need more time of hard works in nuclear science to collect more facts about the real
structure of elementary particles (Fermions QuarksLeptons etc) and composite particles (Hadrons
Baryons Hyperons Nucleons Mesons) They have to improve the optical model which uses optical
laws in its calculation (Fernbach S et al 1949) shell model of Eugene Paul Wigner Maria
Goeppert-Mayer and J Hans D Jensen which uses the Pauli principle to describe the structure of
the nucleus in terms of energy levels (Cohen 1971 Rohlf 1994) and liquid drop model of
Weizsaumlckers formula (Freedman and Young 2004) to reach to an integrated model that combine the
shell model (quantum mechanical) and the collective models
Anyhow the quark theory is still immature to explain the nuclear transformation of the proton
and neutron in a clear way The fundamental particles that form the neutron are still not clear The
quark theory tells us that the neutron is created from three quarks (two down and one up) But the mass
of neutron is not fixed in different nuclei (supposing the proton mass is fixed due to its high stability)
For example the mass of the free neutron in atomic mass units u is (1008665 u) and the mass of
neutron in deuterium is (10062767459 u) and the mass of the neutron in tritium is (10041121177 u)
The nuclear workers said that the decrease in the nuclide mass is converted into the binding energy in
the host nucleus Now we may ask which part of quark of neutron will convert to energy to form the
binding energy when the neutron gets inside the host nucleus
6 Proposal for new nuclear model The proposed nuclear model focus on three main points the outer shell of the nucleus which might be
called the electromagnetic belt (sheath) and the inner new nuclear shell model which might be called
the sphere nuclear shells in addition to modification of the Quark Model of Gell-Mann (Georgi
Eidelman S et al 2004) The aim of the model is to set up a new nuclear model which is capable to
show that the nuclear energy calculation is based on the energy generated by the sub-quark particles
and not on converting some mass of baryons to binding energy
In the present paper we will submit the basic idea of this model and later in the upcoming paper
we will try to give a more detailed structure This crude nuclear model supposes that both the
electromagnetic belt surrounding the nucleus the inner sphere nuclear shells and the sub-quarks
play an important role in nucleus concept We may outline the basic points of this model as below
I- This nuclear model predicts that the protons neutrons and all fermions are composed of integer
multiple of the sub-quarks These sub-quarks are of high magnetic field and align strongly as magnetic
588 Bahjat R J Muhyedeen
dipoles in such a way that they build the fermion in form of N-S dipoles packages Their high magnetic
properties are responsible for the strong nuclear forces We call these magnetic sub-quarks magnetons
In addition there are new elementary particles inside the nucleus which may be called conservon that
keeps both neutron and proton to obey the conservation law and control the conservation of mass
number ∆A=0 linear momentum ∆p=0 total energy ∆E=0 charge ∆Z=0 and spins ∆I=0 during the
nuclear reactions The conservons are also responsible for keeping the mass stability of neutrons and
the proton inside the nuclei The mass of conservon is of integer multiple of the sub-quarks
magnetons mass The binding energy between the proton and the neutron occurs with help from
conservon particles The conservon particles control the nuclear processes The sub-quarks magnetons
and conservons are the main components of the protons and neutrons inside the nuclei
II- The sub-quarks magnetons are the basic building blocks of the fermions The annihilation reactions
of electron-positron are pseudo-annihilation processes The annihilation reactions break the laws of
conservations These pseudo-annihilation reactions are misinterpreted by nuclear workers These
reactions represent inelastic scattering When the electron and the positron collide their
electromagnetic fields will interfere in a deconstructive way (disintegration process) which results in
producing radiation This rule may apply to all matter and antimatter reactions
III- The model predicts that the electromagnetic belt controls the projectile and the target during the
nuclear reactions The electromagnetic belt represents the net charged electromagnetic field of the
nuclear forces of the nuclei We think that the profound understanding of the unfathomable coulomb
barrier surrounding the nucleus is very important The electromagnetic belt is also regulating the
strong nuclear force generated by the magnetons which controls the required mass of the baryon inside
the nuclei and the attraction force of the electrons in the atomic orbitals The charged nuclear forces
will create binding energy of nucleons in the nucleus The source of the binding energy is derived from
the charged nuclear forces rather than from converting some mass of hadrons during the entrance
IV- The model proposed that the protons have certain stable mass while the neutron has several stable
masses that depend on the isotope Z and N The neutron stable mass is available in the stable isotopes
V- The proposed new sphere nuclear shell model states that the nucleus is a composite of many spheres
occupied by 1-4 nucleons and these spheres are distributed among hypothetical nuclear shells It is an
independent-particle nuclear shell model to expect the decay modes and to identify the fertile and
fissile nuclide through shell configuration The sphere has to be filled in the form of (pnpn) ie the
proton first then the neutron next and so on The model explains why some isotopes emit alpha particle
The details of this model will be explained in the forthcoming paper
VI- In the core of the sun or any star this electromagnetic belt of small nuclei became less dense in a
region of high electromagnetic pressure and temperature above 10 million oK In such circumstances
the electromagnetic belt becomes loose (of very low barrier) and the protons and neutrons in their
nuclei are more free to undergo the fusion reactions in equilibrium state (or reversible nuclear
reaction) but the reaction will move toward the stable nuclei of magic numbers when these reactions
occurred at region place little far from the sun core (ie in the circumferences of the core region) which
releases high energies This phase represents a fifth state of matter beyond plasma (where the electrons
are free) in which protons and neutrons are moving more freely in their nuclei This phase is called
ldquoNuclear Transparencyrdquo which endures extra super high temperature and pressure and electromagnetic
field In such Nuclear Transparency phase there is good probability to build the more stable nuclei of
magic number in the sun core such as Fe Ni O Si S Mg C Ne Ca and Cr and even higher nuclides
(actinides) The fifth state may be responsible for the state of hydrostatic equilibrium neither
contracting nor expanding over time
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 589
VII- In the deep core of the sun and stars the nuclei become completely bare of the electromagnetic
belt and the nucleons become free of their nuclei after passing the Nuclear Transparency phase In this
region some of the fermions will be analyzed to their elementary particles the magnetic sub-quarks
magnetons which accumulated in nebulous form and might be called nuclear magma The nuclear
magma starts getting cold and dark because no heat can be absorbed or emitted due to the amorphous
structure The nuclear magma is denser than the nuclei and of high magnetic property and they bind
each other through very strong charged nuclear forces This nuclear magma will be born in the core of
the sun and it moves up toward the surface as ldquocold and darkrdquo mass so called a sunspot These
sunspots (nuclear magma) are collected together through a million of years to form a black hole state
and this nuclear magma state of matter may be called the sixth state of matter The black hole is the
source of the magnetons for creation of elements and then the compounds in the universe When the
star gets old it starts losing its gases and the plasma region will evaporate leaving the cold and
magnetic sunspot alone to form the black hole The number of sunspots in the stars is indicative of the
age of the star The end life of any star is a black hole If a big mass of hydrogen gas will strike the
black hole it will ignite it again to create a new star and so on
This phase ldquonuclear magmardquo is beyond the meta Nuclear Transparency and looks like the
results announced by CERN (European Organization for Nuclear Research) that stated they have
discovered a new state of matter in 2000 which they called quark-gluon plasma It is a phase of
quantum chromodynamics which exists at extremely high temperature andor density and consists of
(almost) free quarks and gluons which are the basic building blocks of matter We can say the CERN
quark-gluon plasma state is a transition state between Nuclear Transparency and the nuclear magma
(finally the black hole) sixth state of matter
VIII- We hope that the workers in nuclear research laboratories try to get a controlling fusion reaction
through three main settings 1- high force of electromagnetic field 2- high pressure 3- flash of high
temperature (Lasergt1018
W) via advanced inertial confinement fusion (AICF) integrated with ion
beam on Deuterium and Tritium nuclei to make their electromagnetic belt more loose in terms of
picoseconds to reach the Nuclear Transparency phase and get a controlled fusion reaction through
controlling the force of the electromagnetic field taking into consideration the Lawson criterion
(Lawson 1957) The trials should go farther than tokamaks and stellarators technology (as in
Torsatron Heliotron and Helias) The stellarator technology lacks high pressure The technologies used
in magnetic confinement fusion and inertial confinement fusion are usually using only two of the three
settings mentioned above thus lessening their efficiency But generally the magnetic field is more
important than the pressure therefore as we expect the future of magnetic confinement fusion
technology is more promising than the inertial confinement fusion The magnetic field is very
necessary to loosen the electromagnetic belts which help the nuclei get into Nuclear Transparency to
undergo fusion reactions
In conclusion the magnetons are basic building blocks of the fermions The protons and
neutrons are composed of the integer multiple of sub-quarks elementary particles magnetons The
protons have certain stable mass and the neutron have several stables masses depending on the isotope
Z and N The conservons control the conservation of mass number linear momentum total energy
charge and spins during the nuclear reactions law of conservations The nuclei in the universe have
been built in the Nuclear Transparency phase with huge binding energies saved in the nuclei and these
energies are liberated during the nuclear processes and no mass will be converted to energy The same
thing happens to nuclear fission and decay processes so no mass will convert to energy or vice versa
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 587
We daily use these stored energies in various chemical and nuclear reactions and there is no mass
converted to energy or vice versa This energy is continuously generated at these two big reservoirs
The speculative equation E=mc2
was misinterpreted when they considered c2 as the conversion
factor from mass to energy The correct understanding is that the head c has to be multiplied with the
mass (mc) to measure the momentum of the particle while next c is considered as the conversion factor
from the momentum unit to the energy unit We will explain this concept in forthcoming paper
4 Energy from chemical reactions In the chemical reactions it is absolutely clear that there is no loss in the mass of the material in any
reaction The process is based on breaking bonds and forming new others The difference in binding
energies which are stored in the atomic orbitals will be released in the case of exothermal reactions In
the case of endothermic reactions we have to supply energy to the electrons of the reactants to help
them to undergo reaction For example the combustion of the hydrocarbon will result in H2O and CO2
5 Energy from nuclear reactions Of course the nuclear visions of nucleus structure and its components is still the greatest obstacle in
the gaining a deep understanding of how can we calculate the energy of nuclear reactions via the
nuclear binding energies like the atomic orbitals far from the mass defect concept The
experimentalists need more time of hard works in nuclear science to collect more facts about the real
structure of elementary particles (Fermions QuarksLeptons etc) and composite particles (Hadrons
Baryons Hyperons Nucleons Mesons) They have to improve the optical model which uses optical
laws in its calculation (Fernbach S et al 1949) shell model of Eugene Paul Wigner Maria
Goeppert-Mayer and J Hans D Jensen which uses the Pauli principle to describe the structure of
the nucleus in terms of energy levels (Cohen 1971 Rohlf 1994) and liquid drop model of
Weizsaumlckers formula (Freedman and Young 2004) to reach to an integrated model that combine the
shell model (quantum mechanical) and the collective models
Anyhow the quark theory is still immature to explain the nuclear transformation of the proton
and neutron in a clear way The fundamental particles that form the neutron are still not clear The
quark theory tells us that the neutron is created from three quarks (two down and one up) But the mass
of neutron is not fixed in different nuclei (supposing the proton mass is fixed due to its high stability)
For example the mass of the free neutron in atomic mass units u is (1008665 u) and the mass of
neutron in deuterium is (10062767459 u) and the mass of the neutron in tritium is (10041121177 u)
The nuclear workers said that the decrease in the nuclide mass is converted into the binding energy in
the host nucleus Now we may ask which part of quark of neutron will convert to energy to form the
binding energy when the neutron gets inside the host nucleus
6 Proposal for new nuclear model The proposed nuclear model focus on three main points the outer shell of the nucleus which might be
called the electromagnetic belt (sheath) and the inner new nuclear shell model which might be called
the sphere nuclear shells in addition to modification of the Quark Model of Gell-Mann (Georgi
Eidelman S et al 2004) The aim of the model is to set up a new nuclear model which is capable to
show that the nuclear energy calculation is based on the energy generated by the sub-quark particles
and not on converting some mass of baryons to binding energy
In the present paper we will submit the basic idea of this model and later in the upcoming paper
we will try to give a more detailed structure This crude nuclear model supposes that both the
electromagnetic belt surrounding the nucleus the inner sphere nuclear shells and the sub-quarks
play an important role in nucleus concept We may outline the basic points of this model as below
I- This nuclear model predicts that the protons neutrons and all fermions are composed of integer
multiple of the sub-quarks These sub-quarks are of high magnetic field and align strongly as magnetic
588 Bahjat R J Muhyedeen
dipoles in such a way that they build the fermion in form of N-S dipoles packages Their high magnetic
properties are responsible for the strong nuclear forces We call these magnetic sub-quarks magnetons
In addition there are new elementary particles inside the nucleus which may be called conservon that
keeps both neutron and proton to obey the conservation law and control the conservation of mass
number ∆A=0 linear momentum ∆p=0 total energy ∆E=0 charge ∆Z=0 and spins ∆I=0 during the
nuclear reactions The conservons are also responsible for keeping the mass stability of neutrons and
the proton inside the nuclei The mass of conservon is of integer multiple of the sub-quarks
magnetons mass The binding energy between the proton and the neutron occurs with help from
conservon particles The conservon particles control the nuclear processes The sub-quarks magnetons
and conservons are the main components of the protons and neutrons inside the nuclei
II- The sub-quarks magnetons are the basic building blocks of the fermions The annihilation reactions
of electron-positron are pseudo-annihilation processes The annihilation reactions break the laws of
conservations These pseudo-annihilation reactions are misinterpreted by nuclear workers These
reactions represent inelastic scattering When the electron and the positron collide their
electromagnetic fields will interfere in a deconstructive way (disintegration process) which results in
producing radiation This rule may apply to all matter and antimatter reactions
III- The model predicts that the electromagnetic belt controls the projectile and the target during the
nuclear reactions The electromagnetic belt represents the net charged electromagnetic field of the
nuclear forces of the nuclei We think that the profound understanding of the unfathomable coulomb
barrier surrounding the nucleus is very important The electromagnetic belt is also regulating the
strong nuclear force generated by the magnetons which controls the required mass of the baryon inside
the nuclei and the attraction force of the electrons in the atomic orbitals The charged nuclear forces
will create binding energy of nucleons in the nucleus The source of the binding energy is derived from
the charged nuclear forces rather than from converting some mass of hadrons during the entrance
IV- The model proposed that the protons have certain stable mass while the neutron has several stable
masses that depend on the isotope Z and N The neutron stable mass is available in the stable isotopes
V- The proposed new sphere nuclear shell model states that the nucleus is a composite of many spheres
occupied by 1-4 nucleons and these spheres are distributed among hypothetical nuclear shells It is an
independent-particle nuclear shell model to expect the decay modes and to identify the fertile and
fissile nuclide through shell configuration The sphere has to be filled in the form of (pnpn) ie the
proton first then the neutron next and so on The model explains why some isotopes emit alpha particle
The details of this model will be explained in the forthcoming paper
VI- In the core of the sun or any star this electromagnetic belt of small nuclei became less dense in a
region of high electromagnetic pressure and temperature above 10 million oK In such circumstances
the electromagnetic belt becomes loose (of very low barrier) and the protons and neutrons in their
nuclei are more free to undergo the fusion reactions in equilibrium state (or reversible nuclear
reaction) but the reaction will move toward the stable nuclei of magic numbers when these reactions
occurred at region place little far from the sun core (ie in the circumferences of the core region) which
releases high energies This phase represents a fifth state of matter beyond plasma (where the electrons
are free) in which protons and neutrons are moving more freely in their nuclei This phase is called
ldquoNuclear Transparencyrdquo which endures extra super high temperature and pressure and electromagnetic
field In such Nuclear Transparency phase there is good probability to build the more stable nuclei of
magic number in the sun core such as Fe Ni O Si S Mg C Ne Ca and Cr and even higher nuclides
(actinides) The fifth state may be responsible for the state of hydrostatic equilibrium neither
contracting nor expanding over time
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 589
VII- In the deep core of the sun and stars the nuclei become completely bare of the electromagnetic
belt and the nucleons become free of their nuclei after passing the Nuclear Transparency phase In this
region some of the fermions will be analyzed to their elementary particles the magnetic sub-quarks
magnetons which accumulated in nebulous form and might be called nuclear magma The nuclear
magma starts getting cold and dark because no heat can be absorbed or emitted due to the amorphous
structure The nuclear magma is denser than the nuclei and of high magnetic property and they bind
each other through very strong charged nuclear forces This nuclear magma will be born in the core of
the sun and it moves up toward the surface as ldquocold and darkrdquo mass so called a sunspot These
sunspots (nuclear magma) are collected together through a million of years to form a black hole state
and this nuclear magma state of matter may be called the sixth state of matter The black hole is the
source of the magnetons for creation of elements and then the compounds in the universe When the
star gets old it starts losing its gases and the plasma region will evaporate leaving the cold and
magnetic sunspot alone to form the black hole The number of sunspots in the stars is indicative of the
age of the star The end life of any star is a black hole If a big mass of hydrogen gas will strike the
black hole it will ignite it again to create a new star and so on
This phase ldquonuclear magmardquo is beyond the meta Nuclear Transparency and looks like the
results announced by CERN (European Organization for Nuclear Research) that stated they have
discovered a new state of matter in 2000 which they called quark-gluon plasma It is a phase of
quantum chromodynamics which exists at extremely high temperature andor density and consists of
(almost) free quarks and gluons which are the basic building blocks of matter We can say the CERN
quark-gluon plasma state is a transition state between Nuclear Transparency and the nuclear magma
(finally the black hole) sixth state of matter
VIII- We hope that the workers in nuclear research laboratories try to get a controlling fusion reaction
through three main settings 1- high force of electromagnetic field 2- high pressure 3- flash of high
temperature (Lasergt1018
W) via advanced inertial confinement fusion (AICF) integrated with ion
beam on Deuterium and Tritium nuclei to make their electromagnetic belt more loose in terms of
picoseconds to reach the Nuclear Transparency phase and get a controlled fusion reaction through
controlling the force of the electromagnetic field taking into consideration the Lawson criterion
(Lawson 1957) The trials should go farther than tokamaks and stellarators technology (as in
Torsatron Heliotron and Helias) The stellarator technology lacks high pressure The technologies used
in magnetic confinement fusion and inertial confinement fusion are usually using only two of the three
settings mentioned above thus lessening their efficiency But generally the magnetic field is more
important than the pressure therefore as we expect the future of magnetic confinement fusion
technology is more promising than the inertial confinement fusion The magnetic field is very
necessary to loosen the electromagnetic belts which help the nuclei get into Nuclear Transparency to
undergo fusion reactions
In conclusion the magnetons are basic building blocks of the fermions The protons and
neutrons are composed of the integer multiple of sub-quarks elementary particles magnetons The
protons have certain stable mass and the neutron have several stables masses depending on the isotope
Z and N The conservons control the conservation of mass number linear momentum total energy
charge and spins during the nuclear reactions law of conservations The nuclei in the universe have
been built in the Nuclear Transparency phase with huge binding energies saved in the nuclei and these
energies are liberated during the nuclear processes and no mass will be converted to energy The same
thing happens to nuclear fission and decay processes so no mass will convert to energy or vice versa
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
588 Bahjat R J Muhyedeen
dipoles in such a way that they build the fermion in form of N-S dipoles packages Their high magnetic
properties are responsible for the strong nuclear forces We call these magnetic sub-quarks magnetons
In addition there are new elementary particles inside the nucleus which may be called conservon that
keeps both neutron and proton to obey the conservation law and control the conservation of mass
number ∆A=0 linear momentum ∆p=0 total energy ∆E=0 charge ∆Z=0 and spins ∆I=0 during the
nuclear reactions The conservons are also responsible for keeping the mass stability of neutrons and
the proton inside the nuclei The mass of conservon is of integer multiple of the sub-quarks
magnetons mass The binding energy between the proton and the neutron occurs with help from
conservon particles The conservon particles control the nuclear processes The sub-quarks magnetons
and conservons are the main components of the protons and neutrons inside the nuclei
II- The sub-quarks magnetons are the basic building blocks of the fermions The annihilation reactions
of electron-positron are pseudo-annihilation processes The annihilation reactions break the laws of
conservations These pseudo-annihilation reactions are misinterpreted by nuclear workers These
reactions represent inelastic scattering When the electron and the positron collide their
electromagnetic fields will interfere in a deconstructive way (disintegration process) which results in
producing radiation This rule may apply to all matter and antimatter reactions
III- The model predicts that the electromagnetic belt controls the projectile and the target during the
nuclear reactions The electromagnetic belt represents the net charged electromagnetic field of the
nuclear forces of the nuclei We think that the profound understanding of the unfathomable coulomb
barrier surrounding the nucleus is very important The electromagnetic belt is also regulating the
strong nuclear force generated by the magnetons which controls the required mass of the baryon inside
the nuclei and the attraction force of the electrons in the atomic orbitals The charged nuclear forces
will create binding energy of nucleons in the nucleus The source of the binding energy is derived from
the charged nuclear forces rather than from converting some mass of hadrons during the entrance
IV- The model proposed that the protons have certain stable mass while the neutron has several stable
masses that depend on the isotope Z and N The neutron stable mass is available in the stable isotopes
V- The proposed new sphere nuclear shell model states that the nucleus is a composite of many spheres
occupied by 1-4 nucleons and these spheres are distributed among hypothetical nuclear shells It is an
independent-particle nuclear shell model to expect the decay modes and to identify the fertile and
fissile nuclide through shell configuration The sphere has to be filled in the form of (pnpn) ie the
proton first then the neutron next and so on The model explains why some isotopes emit alpha particle
The details of this model will be explained in the forthcoming paper
VI- In the core of the sun or any star this electromagnetic belt of small nuclei became less dense in a
region of high electromagnetic pressure and temperature above 10 million oK In such circumstances
the electromagnetic belt becomes loose (of very low barrier) and the protons and neutrons in their
nuclei are more free to undergo the fusion reactions in equilibrium state (or reversible nuclear
reaction) but the reaction will move toward the stable nuclei of magic numbers when these reactions
occurred at region place little far from the sun core (ie in the circumferences of the core region) which
releases high energies This phase represents a fifth state of matter beyond plasma (where the electrons
are free) in which protons and neutrons are moving more freely in their nuclei This phase is called
ldquoNuclear Transparencyrdquo which endures extra super high temperature and pressure and electromagnetic
field In such Nuclear Transparency phase there is good probability to build the more stable nuclei of
magic number in the sun core such as Fe Ni O Si S Mg C Ne Ca and Cr and even higher nuclides
(actinides) The fifth state may be responsible for the state of hydrostatic equilibrium neither
contracting nor expanding over time
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 589
VII- In the deep core of the sun and stars the nuclei become completely bare of the electromagnetic
belt and the nucleons become free of their nuclei after passing the Nuclear Transparency phase In this
region some of the fermions will be analyzed to their elementary particles the magnetic sub-quarks
magnetons which accumulated in nebulous form and might be called nuclear magma The nuclear
magma starts getting cold and dark because no heat can be absorbed or emitted due to the amorphous
structure The nuclear magma is denser than the nuclei and of high magnetic property and they bind
each other through very strong charged nuclear forces This nuclear magma will be born in the core of
the sun and it moves up toward the surface as ldquocold and darkrdquo mass so called a sunspot These
sunspots (nuclear magma) are collected together through a million of years to form a black hole state
and this nuclear magma state of matter may be called the sixth state of matter The black hole is the
source of the magnetons for creation of elements and then the compounds in the universe When the
star gets old it starts losing its gases and the plasma region will evaporate leaving the cold and
magnetic sunspot alone to form the black hole The number of sunspots in the stars is indicative of the
age of the star The end life of any star is a black hole If a big mass of hydrogen gas will strike the
black hole it will ignite it again to create a new star and so on
This phase ldquonuclear magmardquo is beyond the meta Nuclear Transparency and looks like the
results announced by CERN (European Organization for Nuclear Research) that stated they have
discovered a new state of matter in 2000 which they called quark-gluon plasma It is a phase of
quantum chromodynamics which exists at extremely high temperature andor density and consists of
(almost) free quarks and gluons which are the basic building blocks of matter We can say the CERN
quark-gluon plasma state is a transition state between Nuclear Transparency and the nuclear magma
(finally the black hole) sixth state of matter
VIII- We hope that the workers in nuclear research laboratories try to get a controlling fusion reaction
through three main settings 1- high force of electromagnetic field 2- high pressure 3- flash of high
temperature (Lasergt1018
W) via advanced inertial confinement fusion (AICF) integrated with ion
beam on Deuterium and Tritium nuclei to make their electromagnetic belt more loose in terms of
picoseconds to reach the Nuclear Transparency phase and get a controlled fusion reaction through
controlling the force of the electromagnetic field taking into consideration the Lawson criterion
(Lawson 1957) The trials should go farther than tokamaks and stellarators technology (as in
Torsatron Heliotron and Helias) The stellarator technology lacks high pressure The technologies used
in magnetic confinement fusion and inertial confinement fusion are usually using only two of the three
settings mentioned above thus lessening their efficiency But generally the magnetic field is more
important than the pressure therefore as we expect the future of magnetic confinement fusion
technology is more promising than the inertial confinement fusion The magnetic field is very
necessary to loosen the electromagnetic belts which help the nuclei get into Nuclear Transparency to
undergo fusion reactions
In conclusion the magnetons are basic building blocks of the fermions The protons and
neutrons are composed of the integer multiple of sub-quarks elementary particles magnetons The
protons have certain stable mass and the neutron have several stables masses depending on the isotope
Z and N The conservons control the conservation of mass number linear momentum total energy
charge and spins during the nuclear reactions law of conservations The nuclei in the universe have
been built in the Nuclear Transparency phase with huge binding energies saved in the nuclei and these
energies are liberated during the nuclear processes and no mass will be converted to energy The same
thing happens to nuclear fission and decay processes so no mass will convert to energy or vice versa
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 589
VII- In the deep core of the sun and stars the nuclei become completely bare of the electromagnetic
belt and the nucleons become free of their nuclei after passing the Nuclear Transparency phase In this
region some of the fermions will be analyzed to their elementary particles the magnetic sub-quarks
magnetons which accumulated in nebulous form and might be called nuclear magma The nuclear
magma starts getting cold and dark because no heat can be absorbed or emitted due to the amorphous
structure The nuclear magma is denser than the nuclei and of high magnetic property and they bind
each other through very strong charged nuclear forces This nuclear magma will be born in the core of
the sun and it moves up toward the surface as ldquocold and darkrdquo mass so called a sunspot These
sunspots (nuclear magma) are collected together through a million of years to form a black hole state
and this nuclear magma state of matter may be called the sixth state of matter The black hole is the
source of the magnetons for creation of elements and then the compounds in the universe When the
star gets old it starts losing its gases and the plasma region will evaporate leaving the cold and
magnetic sunspot alone to form the black hole The number of sunspots in the stars is indicative of the
age of the star The end life of any star is a black hole If a big mass of hydrogen gas will strike the
black hole it will ignite it again to create a new star and so on
This phase ldquonuclear magmardquo is beyond the meta Nuclear Transparency and looks like the
results announced by CERN (European Organization for Nuclear Research) that stated they have
discovered a new state of matter in 2000 which they called quark-gluon plasma It is a phase of
quantum chromodynamics which exists at extremely high temperature andor density and consists of
(almost) free quarks and gluons which are the basic building blocks of matter We can say the CERN
quark-gluon plasma state is a transition state between Nuclear Transparency and the nuclear magma
(finally the black hole) sixth state of matter
VIII- We hope that the workers in nuclear research laboratories try to get a controlling fusion reaction
through three main settings 1- high force of electromagnetic field 2- high pressure 3- flash of high
temperature (Lasergt1018
W) via advanced inertial confinement fusion (AICF) integrated with ion
beam on Deuterium and Tritium nuclei to make their electromagnetic belt more loose in terms of
picoseconds to reach the Nuclear Transparency phase and get a controlled fusion reaction through
controlling the force of the electromagnetic field taking into consideration the Lawson criterion
(Lawson 1957) The trials should go farther than tokamaks and stellarators technology (as in
Torsatron Heliotron and Helias) The stellarator technology lacks high pressure The technologies used
in magnetic confinement fusion and inertial confinement fusion are usually using only two of the three
settings mentioned above thus lessening their efficiency But generally the magnetic field is more
important than the pressure therefore as we expect the future of magnetic confinement fusion
technology is more promising than the inertial confinement fusion The magnetic field is very
necessary to loosen the electromagnetic belts which help the nuclei get into Nuclear Transparency to
undergo fusion reactions
In conclusion the magnetons are basic building blocks of the fermions The protons and
neutrons are composed of the integer multiple of sub-quarks elementary particles magnetons The
protons have certain stable mass and the neutron have several stables masses depending on the isotope
Z and N The conservons control the conservation of mass number linear momentum total energy
charge and spins during the nuclear reactions law of conservations The nuclei in the universe have
been built in the Nuclear Transparency phase with huge binding energies saved in the nuclei and these
energies are liberated during the nuclear processes and no mass will be converted to energy The same
thing happens to nuclear fission and decay processes so no mass will convert to energy or vice versa
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
590 Bahjat R J Muhyedeen
7 The nature of electromagnetic radiation1
The wave nature of electromagnetic radiation was first mathematically formulated by James Clerk
Maxwell in 1861 the Scottish mathematician and theoretical physicist [On physical lines of forcerdquo]
(Maxwell 1861) and in 1865 [ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo] (Maxwell 1865)
which reformulated by Oliver Heaviside and subsequently confirmed by the German physicist and
mechanic Heinrich Hertz in 1887 (Hertz1887) The electric and magnetic fields obey the properties
of superposition such as refraction and diffraction The main aspect of the nature of light is the
frequency Electromagnetic radiation carries energy through frequency which may be important when
it interacts with matter through interference The great success of Max Planck in treating the black
body radiation is due to his adoption of Boltzmannrsquos idea of statistical interpretation of the second law
of thermodynamics (the entropy) in 1877 that the wave consists of discrete packets of energy
(Boltzmann 1877) So Planck treated the vibrational energy of the resonator as discrete packets of
energy to simplify the treatment in a similar manner to that of the kinetic gas theory He was deeply
suspicious of his treatment and said that ldquoMy unavailing attempts to somehow reintegrate the action
quantum into classical theory extended over several years and caused me much troublerdquo Really he did
not aim to quantize the energy but his treatment was completely correct due to the emitted fixed
frequencies of the monochromatic light The emission spectra are quantized in nature due to the
electron-nucleus structure Therefore at that time in 1900 he did not realize that he revealed a great
fact on the atomic structure from a quantization point of view
Unfortunately these suggested wave-packets were misinterpreted by Einstein in 1909 as small
zero mass particles which must have well-defined momenta (hνc) and act in some respects as
independent point-like particles which were called photons in 1926 by the physical chemist Gilbert
Lewis and confirmed that ldquothe energy and momentum of light are concentrated in particlesrdquo (Einstein
1909) Actually Einstein was incorrect and these packets are still waves in nature
The gravitational redshift which based on the particle theory of light is also incorrect because
the nuclear materials of stars are full of magnetic property that interferes with magnetic vector of light
and not due to particulate property (photons) of light This misinterpretation by Einstein (Einstein
1911) also lead Compton (Compton 1923) and De Broglie to misbelieve that the light is of dual
character (De Broglie 1924)
As we think that the source of any light whether from sun or from our artificial sources is no
more than an emission spectra In this process the electrons of the atoms and molecules absorb energy
become excited jump to higher levels and then they get down emitting the electromagnetic radiation
These processes of jumping up and falling down will generate a series of waves (like heart pulses) and
not continuous electromagnetic wave The energy of these pulses is represented by their frequencies
Thus these discrete packets of energy are still waveform in nature and we may call each of these
discrete packets of energy as frequentons to differentiate them from discrete packets of photons of
particle nature The same thing can be said for gamma which is emitted from the nuclear energy levels
as energy quanta (frequentons) Subsequently the light does not need an energy carrier like photons
but it transfers its energy to the matter through interference We can say that ldquoThe energy of light that
1 From a particle theory point of view Reneacute Descartes (1596-1650) declared that light was a disturbance of the
plenum the continuous substance of which the universe was composed Pierre Gassendi (1592-1655) an atomist proposed
a particle theory of light which was published posthumously in the 1660s Isaac Newton studied Gassendis work at an early
age and preferred his view to Descartes theory of the plenum He stated in his Hypothesis of Light of 1675 that light was
composed of corpuscles (particles of matter)
From a wave theory point of view Robert Hooke published a wave theory of light in 1660s Christiaan Huygens
worked out his own wave theory of light in 1678 and published it in his Treatise on light in 1690 He proposed that light
was emitted in all directions as a series of waves in a medium called the luminiferous ether As waves are not affected by
gravity it was assumed that they slowed down upon entering a denser medium
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 591
propagate as a ray is not continuously distributed over steadily increasing spaces but it consists of a
finite number of energy quanta called frequentons which is absorbed and emitted as entitiesrdquo
In the sun the source of energy are the nuclear reactions (mainly fusion and rarely fission)
which emit gamma rays in energy quanta based on the shell model (spin-orbit interaction model) that
will strike the atoms of the gases that result in light This light when entering our atmosphere will strike
the electrons of all molecules of gases Molecules can absorb and emit light through its electrons Once
a molecule has absorbed light (energy) the molecule can rotate translate vibrate and undergo
electronic transition which leads to a full spectrum due to the electronic vibrational and rotational
energies of the molecules The rotation motion will increase the microwave background in the
universe
8 Notes on photoelectric effect The reason for creation the concept of particle behavior for electromagnetic radiations was due to the
erroneous explanation of photoelectric effect When Einstein interpreted the photoelectric effect
phenomenon using the particle concept in light his work was accepted at that time in 1905 because the
nucleus structure was not discovered until the work of Ernest Rutherford in 1911 The fundamental
picture of nucleus was completed in 1934 after the discovery of the neutron (Rutherford 1904-1933)
So in 1905 there was an unclear picture or vision about the atom and how the electrons are bound
with the nucleus and moving in specific orbital of quantized nature that results in absorption and
emission in specific frequencies based on the Bohr model (Bohr 1913) The zero mass photons could
not transfer the energy to the electrons through impact as its momentum is zero In spite of the
improper mechanism of the photon to explain the photoelectric effect the formula used by Einstein for
the photoelectric effect is still valid but in view of frequentons as follow
hf=Φ +EKmax
h is Planckrsquos constant f is the frequency of the incident frequenton Φ=hfo is the work function
(or W) EKmax =12m 2
mv the maximum kinetic energy of ejected electrons
fo is the threshold frequency for the photoelectric effect to occur m is the rest mass of the
ejected electron and 2
mv is the velocity of the ejected electron
In conclusion Einstein was obliged to use quantized particles such as photons to interpret the
photoelectric effect phenomenon because he did not realize at that time the energies of the electrons are
quantized in their atomic orbitals The success of Einstein in his treatment was not attributed for
photons proposal but for two main reasons 1- The use of the Max Planck conversion factor h and 2-
The real quantized nature of electrons (ie absorb and emit energy in quantized energies due to the
quantized levels of energy)
Based on our understanding we can interpret this photoelectric effect phenomenon from the
wave point of view energy frequenton that the traveling electromagnetic wave frequentons
incidents on atomic structure (even in crystal form) induces oscillation in the atom and result in
electrons excitation If the frequency (energy) of incident frequenton is equal to or larger than that of
the bound electron it will leave the atom with kinetic energy This process will take place through the
interference mechanism (ie obeys the superposition law of the light electric and magnetic vectors with
matter corresponding vectors of its electrons electric and magnetic vectors as a simple vector addition)
The simplest conception is that a light quantum frequenton transfers its entire energy to a single
electron through interference Finally we can say that the electromagnetic spectrum is a pure wave and
does not have dual character like electrons and any small charged particles
The use of the Max Planck conversion factor h also lead to success of the Bohr and
Schroumldinger theoretical treatments (Bohr 1913 Schroumldinger 1926) in spite of their different adoptions
such as the particle and wave concepts respectively Although Schroumldinger had made several
approximations on his theoretical treatments but the final solutions gave inaccurate description to the
final calculated orbitalrsquos functions especially in the molecular system due to inadequate wave
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
592 Bahjat R J Muhyedeen
concepts In the thirties of twentieth century Slater (Slater 1960) and Clementi and Raimondi in 1963
(Clementi and Raimondi 1963 1967) treated the screening effect and effective Z to improve the
functions of the bases sets of Schroumldinger solutions Several basis sets have been published later to
describe the electrons in their orbits including such corrections The bound electron is affected by the
quantum defects D and other parameters such as the effective Z and N
The most update values for D
Z and N
were calculated and extended to radon by Derwish etal (Muhyedeen Al-Thib and Derwish
1993) and they are more accurate than those of Slater and Clementi values
9 The dual character of electrons-like particles As we discussed above the electron is a charged particle and when it moves it will generate a magnetic
field perpendicular on the electric field The resulted electromagnetic field is an inherent property and
it will affect its behavior and gives the electron the wave nature From this point of view it will show a
dual character But this behavior does not mean it converts from a particle form to a wave form or vice
versa Possibly only fermions can show this property and obeyed the De Broglie formula λ=hp The
process of generating the negative or positive charge to the electron depends on the wave configuration
deduced from the net electromagnetic field of its flexible mass
Of course the electron diffraction pattern showed by Clinton Davisson and Lester Germer in
Bell Lab in 1927 (Davisson 1937 1965) was due to the inherent electromagnetic field of the electron
and not to the electron mass itself The Fresnel diffraction and specular reflection of neutral atoms
could be related to their electron electromagnetic clouds (Oberst et al 2005 Goodman 1996) We think
that the atoms look like spongy spherical balls in their behavior due to the great electromagnetic field
of their electrons and they show great elasticity and wave character through any impact
The new concept submitted by De Broglie of wave character of the electron led Erwin
Schroumldinger to overdo in wave nature of the electron and created the wave mechanic and described
the electron by pure wave nature which resulted in some errors in the final calculations Of course
Einstein in his late age 1950 believed with the wave nature of the electron to confirm the
deterministic character of the measurement and to defeat the probabilistic principles of Copenhagen of
Bohr and Heisenberg but he forgot that the wave nature of the electron will spoil the photoelectric
effect mechanism between the electron and the photon We can say the idea that the electron is of pure
wave nature is nonsense because if the electron nature is really pure wave without mass density then
the material structure will depend on the nuclei of small size and the universe will be in a different
style Furthermore if the electron is wave to whom the mass (me=9109x10-31
Kg) belongs Is it to the
wave
In conclusion the electron has a mass therefore it behaves as a particle and it has an
electromagnetic field thus it behaves as wave
10 Notes on Comptonrsquos effect Arthur Compton was incorrect when he used the particle character of light the photons in his
derivation in addition to that he used mec2 to describe the electron energy in the atom which does not
describe well the electron energy Eγ+Ee= Eγ+Ee where Ee=mec2
(Compton 1923)
We can easily interpret the Comptonrsquos effect through the reaction of the quantum of light
(frequentons) with the dual character of the circulating electron through its mass and its inherent
electromagnetic field Then the electron will absorb the energy of the incident frequenton through its
electromagnetic field and it recoils while the other frequentons will interfere with the electromagnetic
field and endures reflection based on the electromagnetic field of the electron direction In this process
we do not need the particle character of light represented by photons So neither the photoelectric
effect nor the Comptonrsquos effect need light photons to be understood or interpreted Of course other
charged particle will show the same dual property I prefer to rewrite the Comptonrsquos equation using the
universal particle speed constant b (see Section 14) instead of c speed of light as follow
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 593
thus the corrected Compton wavelength will equal to 112496 x 10
-11 m
rather than 243 x 10-12
m In the next paper we will explain the new understanding for this λ
11 Notes on Heisenberg uncertainty principle Since the uncertainty of Heisenberg (Heisenberg 1927) is based on the deflection of the electron by
the photon in Comptonrsquos effect therefore this principle become less accurate because of an incorrect
concept of the particular behavior of the photon Heisenberg thought at the time that the incident
photon will immediately impact the electron and causes it to shift he said that ldquothe reflected photon
will change the momentum of the atom by an uncertain amount inversely proportional to the accuracy
of the position measurementrdquo
But as we explained in the previous paragraph light does not have photons to impact and
deflect the electron Instead we can say that when the frequenton interact with the electromagnetic
field of the electron of the matter there is enough time to measure the position and the momentum of
the electron and currently we can talk about the new concept of the certainty principle as follows
The origin of the uncertainty principle came from the theorem in the Fourier analysis That the
standard deviation of the square absolute value of a function ltF2gt times the standard deviation of the
square absolute value of its Fourier transform is at least lt116π2gt (Folland and Sitaram theorem 11
ltF2gt lt116π
2) =1 if we take the square root of both sides we will get rarr ltFgt= (14π) In the wave
treatment the uncertainty in the wave number ύ with position x of wave is a well-known formula
ΔxΔύ =14π If we use De Broglie formula to get ύ value as ph then we get (ΔxΔp) ge h4π which
represents the Heisenberg uncertainty principle
Finally we can surely say that the position and the momentum can certainly be measured and
the value of (ΔxΔp) = h4π will give the exact value due to the interference of waves
12 Does radiation have mass Most scientists during the period 1890-1910 predict that the body loses some of its weight after
radiation Max Planck in 1907 reported after a deep investigation that ldquoThe inertia mass of body is
altered by absorption or emission of heat energy The increment of mass of body is equal to heat
energy divided by square of speed of light [(m-M)=Ec2]rdquo (Planck 1907 1908) Einstein also in 1909
showed in his paper The Development of Our Views on the Composition and Essence of Radiation
that the inertial mass of an object decreases by (Lc2) when that object emits radiation of energy L
(Einstein1909)
Of course this concept again is incorrect because all types of energy have zero mass The heated
mass as long as it has been supplied by any energy source such as heating or electric potential radiates
emission spectra in the form of light with various frequencies as an electromagnetic radiation but it
does not lose any mass In other clear words the excited electrons will emit the absorbed energy and
there is no mass loss during radiation
13 Non-relativistic quantum mass-energy equivalence E=mbc We have explained above that the concept of conversion of mass to energy or vice versa are incorrect
The experimentalists and the theoreticians need more time to improve the theories that enable them to
calculate the actual nuclear forces and binding energies for the nuclides from their substructure
Regarding nuclear reactions calculations we use the speculative Einsteinrsquos mass-energy equivalence
formula E=mc2 which usually overestimates the nuclear energies In this regard we would like to
suggest a novel non-relativistic formula with a new conversion factor other than (c2) to help in the
calculation of nuclear energy
The treatment of black body radiation by Max Planck (Planck 1901) disclosed to us a fact that
the energy of the electrons in the atomic orbital are quantized From a physical point of view the peaks
of the thermal radiation of black body cover the range 400-800 nm (31-155 eV) which is below the IP
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
594 Bahjat R J Muhyedeen
(eV) of any elements in the periodic table (IPCs= 389 eV) That means this thermal radiation is a type
of a condensed atomic emission radiation The energy of the thermal radiation was calculated by Max
Planck using the two universal constants (hPlanck= 662606957x10-34 Jsec) (kPlanck= 13806488x10
-23
JoK) which is given by E=hν and E=kT (please note that this constant kPlanck is improperly known in
the literature as Boltzmann2) The success of the Max Planck treatment which results in finding the
two constants hPlanck and kPlanck was based on three assumptions that the energy is quantized the
temperature θ is set to one Kelvin and the wavelength at its max value These three assumptions and
others such as Thiesen Stirlingrsquos theorem Kurlbaum empirical formula led him to a historical success
of black body radiation In the present treatment we followed some Planckrsquos assumptions to find the
new converting factor (through the novel mass-energy equivalence formula) We will derive the new
formula which will be based on the following points first - experimental principles second - semi-
empirical formula third - wave quantized character (energy frequenton) and fourth - universal
constants that reflect the frequentons characters which were called energy quanta by Max Planck
We may start from the relation between the temperature of the black body radiation and the
energy through the second constant kPlanck as follow
E=kPlanck
Tblackbody
(1)
The temperature of the thermal spectral of black body is well related with the wavelength of the
emitted radiation The relation between T and λmax (at high frequencies) is well described by Wienrsquos
displacement law (Mehra1982) which states that there is an inverse relationship between the
wavelength of the peak of the emission of black body and its temperature at equilibrium state as
follow
(2)
Where
is the peak wavelength in meter of the emission spectra at equilibrium
T is the temperature of the blackbody in Kelvinrsquos (oK) and
b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551x10-3
meter-Kelvin Hence we have
or
2 Of course the kPlanck constant is calculated by Max Planck through his treatment of black body radiation when he used
the entropy equation as appeared in his reprint in item 2 eq=3rdquo as follow
sect2 We now set the entropy SN of the system proportional to the logarithm of its probability W within an arbitrary additive
constant so that the N resonators together have the energy EN
(3) SN = k log W + constant
And in item 11 in eq no 14 he related both h and k as appeared in his reprintrdquo
(14) k4h
4 = 11682 x 10
15
And in item 12 he related both h and k in another formula as appeared in his reprint as follow
hk=(49561 x 0294)31010
=4866 x 10-11
From these two formulas he got k and h values
In the literature this kB is called Boltzmann constant (which is given by RNA ie the gas constant divided by the Avogadro
constant where R=kNA it is improper assignment due to trivial substitution loop ie k=kNANA) and this equation SN = k
log W + constant is called Boltzmann equation Planck used this formula and calculated the k constant with h constant Of
course Planck mentioned in his paper that such expression was used by L Boltzmann for a similar idea Planck said in
his Nobel Prize lecture in 1920 ldquoThis constant is often referred to as Boltzmanns constant although to my knowledge
Boltzmann himself never introduced itrdquo
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 595
Wien considered the thermal emission as an adiabatic process which means the waves of light is in
thermal equilibrium state3 Wien showed that the energy of cavity light changes in exactly the same
way as the frequency Wienrsquos law born due to the quantization of the atomic orbital but it was very
early for Wien to understand it If we substitute equation no4 into equation no1 we get
When the radiation energy is in equilibrium with the temperature this means that the emitted
energy from the electron is equal to the absorbed energy We think that the electromagnetic field EMF
of the electron absorbs and emits the electromagnetic energy through interference of both fields but the
electron EMF is confined by its mass m due to its magnetons Thus the wavelength λmax in eq no 5
belongs to energy absorbed by the EMF of the excited electrons The wavelength λmax of the excited
EMF and the mass m of the electrons are well related through the formula of duality The proper
relationship between m and λ is coming from De Broglie expression4 (De Broglie 1924) which relates
the wavelength and the momentum of the particles through Planck constant hPlanck Thus we can write
p = hPlanck
λmax (6)
Or
λmax = hPlanck
P (7)
The momentum of any high speed particle might be described by speed of light and can be given by the
following equation
p=mc (8)
where
m is the mass of the particle and
c is the velocity of light equals to 299792458 x 108 ms
We may substitute the value of momentum p from eq no 8 into the wavelength of the black body in
eq no 7 to get
And by substituting the value of the wavelength by its corresponding momentum from eq no 9 into
eq no5 we get
Substituting the value for kplanck which is known as Boltzmann constant kB in eq no 10 we get
Or
(12)
The derived equation may be rewrite as a general formula in form of E=(mb)c where (mb) is the
momentum of the particle and c is a conversion factor from momentum unit to energy unit or as
follow
E=mbc (13)
Now we can write the mass-energy equivalent as follow
3 Of course the b is a constant of proportionality called Wienrsquos displacement constant and equals 2897768551 x10
-3
meter-Kelvin which can be given by (hck)4965114 If you use these constants (hck) directly and not from Wien b
constant then you will get a similar formula E=(14965114) x mc2 or E=02014 x mc
2
4 We have a different understanding for De Broglie which will be published in details in the next paper where we think that
this wavelength represents the excited radius of the fermion
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
596 Bahjat R J Muhyedeen
(
)
The mass-energy equivalence will gets its final value if we substitute for the speed of light 299792458
x108 ms as follow
For one atomic mass unit u the mass-energy equivalent is calculated as follow
1u = (1660538921 x 10-27
kg) x (1810137886817 x 1016
Jkg) (16)
1u = 30058 x10-11
J (17)
The equivalent energy to one u in MeV is calculated as follow
1 u (in MeV) = 30058x10-11
J x MeV160218x10-13
J (18)
Or
1 u = (187607) MeV (19)
A different value for Planck constant kPlanck (1429x10-23
J o
K)5 mentioned in the literature and
the corresponding value of universal particle speed constant equals b=0624942x108 ms which gives
an equivalent energy equal to194177 MeVu
Relating our value of the mass-energy equivalence in MeV from eq no 19 with that of
Einstein we get the following the ratio of mbcmc2 which equals to (187607 MeV 93149 MeV) =
020141 We may use our mass-energy equivalent of (Em) from our equation E=mbc in relation to the
speculative equation of Einstein E=mc2
in the calculation of the energy released from nuclear fission
Practically Einstein equation E=mc2
usually overestimates the Q-value while the max efficiency
achieved in nuclear reactors (ie SCWR) and weapons is 45 In the laboratory it is confirmed
(Hambsch1989 Thiereus 1981) that using thermal neutrons the Total Kinetic Energy (TKE) of fission
fragments (of the mass=355x10-28
Kg) that results from of 235
U and 239
Pu is 20-60 MeV less than Q-
value of reaction predicted by Einsteinrsquos equation E=mc2 (200MeV for
235U) The typical plot of the
distribution of the total of the kinetic energy of 235
U or 239
Pu shows a peak at 175 MeV Bakhoum has
attempted to calculate the TKE using the wave mechanical equation H=mv2 and he got 45 MeV at
v=45x107
ms (Bakhoum 2002) Some alternate suggestions have been made to explain the total
kinetic energy of fission fragments by extending the successful Liquid-Drop Model of Bohr and
Wheeler (Straede 1987 Wilkins 1976)
The Q-value for fission fragments6 of
is estimated based on the new mass-energy
equivalence E=∆mbc where ∆m is the mass defect to be 3482 MeVbc In the forthcoming paper we
will use E=mbc to calculate all types of nuclear reactions The energies of fission of are
compared with others as seen in Table-1
Table-1 The theoretical Q-value for fission reaction
The Experimental Value (Hambsch1989Thiereus 1981)
From Gaussian graph
(in lab)
From E=∆mbc (See footnote 6 )
From E=mc2
(Einstein1905)
From H=mv2
(Bakhoum2002)
140 -180 MeVc2
175 MeVc2 3720 MeVbc
4113 MeVbc
1847 MeVc2
2042 MeVc2
45 MeVv2
5 This value is the corrected value derived in 2007 by a mathematician The author has re-manipulated the statistical model
of the combinational theory which used by Max Planck and gave this k value Another source is from this link
httpdbhswvusdk12causwebdocsChem-HistoryPlanck-1901Planck-1901html
6The Q-value for
is equal to 3482 MeVbc the Q-value for
is equal to 3721 MeVbc and the Q-value for
is equal to 4113 MeVbc
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 597
14 Some derived equations for non-relativistic particles As we explained the b constant is a universal particle speed constant which represents the optimum
speed of the electron in the atomic orbitals and of all elemental particles that are emitted through all
nuclear reactions and processes and no particle can exceed this value unless it is accelerated Therefore
this speed constant b can be used to calculate the momentum of the fermions as shown below
p=mb (20)
The corresponding mathematical kinetic energy for momentum p=mb of the heavy particle can be
given by E=mb2 while the electromagnetic field EMF (energy) generated by the particle can be given
by following equation
E=mbc (21)
Equation no 21 can be used for the calculation the EMF generated by the fermions We can write a
novel equation similar to the De Broglie equation for non-relativistic relations to describe the
frequency of the EMF of the fermion as follows
(22)
The universal particle speed constant b can be used also to relate the wavelength and the frequency of
the EMF of the fermion as below
b=λυ (23)
The equation no 23 can be used in particle physics for any fermion moving with velocities less than
speed of light Now in particle physics we have c=λυ for wave and b=λυ for EMF of the particle The
charged EMF of the fermion is described by the universal particle speed constant b The non-
relativistic equivalent energy of the EMF of the fermion can be calculated as follows
E=hbλ (24)
The kinetic energy of heavy particle also can be calculated from its mass as follows
E=mb2 (25)
The energy of fission products or decay processes which are accompanied by neutrinos can be
calculated from the mass defect ∆m as follows
E=∆mbc (26)
We may apply the above equations to calculate the momentum p value for excited electron in atomic
orbital as follows
p=meb (me=910938291 x 10-31
Kg b= 0603797 x108 ms)
p=0603797 x 108 ms x 910938291 x 10
-31 Kg
p=550021807290927 x 10-23
Kg ms
The frequency of the electron EMF generated by its mass can be calculated from equation no 22 This
EMF dissipates only when it impacts the positron and result in the disintegration process
= 24909 x 10
18 Hz (in region of Gamma-ray)
The wavelength of the electromagnetic field of electron can be calculated from equation no 23 b=λυ as
follow
λ=bυ = 24240 x 10-12
m or 2424 picometer (in region of γ-ray which is identical to Comptonrsquos λ)
This wavelength (2424 pm) is depending on the electron mass and the universal particle speed
constant b It describes the strength of the charged EMF of the electron itself which is ready to absorb
and emit energy as seen in the derivation of E=mbc It is different from the wavelength that is
corresponding to the momentum of the electron with speed b Our interpretation to the wavelength
given by λ=hmb is to represents the excited radius of the fermion mass due to the flexibility of the
sub-structure (magnetons) of the fermion and not due to the duality concept For example the active
radius of the electron is given by the following equation
= 120438 x 10
-11 m or 012 picometer (which is close to primitive Bohr radius 529 x 10
-11 m)
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
598 Bahjat R J Muhyedeen
Finally we can say that there are three difference concepts for the energy given by the E=mbc The first
meaning for E=mbc is to describe the mathematical energy corresponding to the momentum p=mb of
the fermion In current physics this energy is described by the kinetic energy formula E=1mv2 The
second meaning for the energy given by the E=mbc is to describe the energy generated by the fermion
The third meaning for the energy given by the E=mbc is to describe the energy of any nuclear reaction
or decay process such beta decay which may be calculated directly from E=Δmbc where Δm is the
mass defect (see Table-1)
15 b-constant components The two components of the light or the electromagnetic ray namely the magnetic constant μo and
electric constant εo7
are related to the speed of light due to Maxwell formula as follow
oo
c
1 εo= 8854187817 x 10
-12 Fm μo= 1256637061 x 10
-7 NA
2 (27)
Therefore we can re-write the Maxwell formula for universal particle speed constant b and
calculate the magnetic component for the charged EMF of the fermion Here we suppose that the value
of electric constant εo is fixed due to the fixed electric charge while the value of the magnetic constant
μo will be changed and increased for these charged fermions or particles Consequently we can
calculate the new magnetic constant μb for the charged particle as follow
radic or
(28)
The calculated value of from equation no 28 is equal to 30979 x 10-5
NA2 which is larger
than that of magnetic constant μo=1256637061 x 10-7
NA2 of the electromagnetic waves by 2465
times and this gives a special magnetic property to the field of the charged particles The interaction of
the magnetic component of the charged particle with the exerted magnetic field will be stronger than
that of electromagnetic waves based on Lorentz force F=q[E+vxB] or F=q[E+vxμbH] This concept
explains the variance of the deflection of alpha beta and gamma through passing the magnetic field It
also explains the strong bonds in the chemical interactions which are attributed to the strong
interference of the charged electromagnetic field of the electrons Of course this concept is novel in
field of electrodynamics quantum science
16 Summary and concluding remarks We have discussed the idea of conversion of mass to energy and vice versa and we showed it is
incorrect both in the chemical and in the nuclear reactions We showed that the radiating body will not
lose any mass A new nuclear model is proposed The model predicts that the protons neutrons and all
fermions are composed of integer multiple of sub-quarks basic building blocks of matter called
magnetons This model proposes also a new elementary particle called conservons These conservons
are responsible for keeping the mass stability of neutrons and the proton inside the nuclei We also
proposed the fifth and sixth states of matter in the stars The fifth state represents the nuclear
transparency in which the nuclear components are loosely bound and free to endure a nuclear reaction
due to the weakness of the electromagnetic belt The sixth state represents the nuclear magma in
which there are no nuclei identities but only magnetons particles that combined with each other
through very strong forces The nuclear magma will be collected later as black holes The nature of
light has been discussed and explained to be composed of wave discrete packets of frequentons to
differentiate them from discrete packets of photons of particle nature We concluded that light is not of
7 All physical constants used in this article are taken from httpphysicsnistgov which depends on the Committee on Data
for Science and Technology (CODATA) values
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 599
dual character and unlike the fermion We also explained both the photoelectric effect and Comptonrsquos
effect based on the new wave concept of light represented by frequentons We attributed the duality of
the fermions due to their charged electromagnetic field and their flexible structure of the magnetons
Finally we derived a novel semi-empirical formula for non-relativistic mass-energy
equivalence E=mbc where b is universal particle speed constant equals to 0603797 x 108 ms This
speed constant is equal to 020141 of speed of light In our opinion that this derived universal particle
speed constant represents the optimum speed to be reached by the non-accelerated moving charged or
uncharged particles or fermions The concept of this semi-empirical formula will refute the relativity
idea of relative mass time dilation length contraction and other ideas of relativity Finally we can use
this universal particle speed constant to relate the wavelength and the frequency of the elementary
particles in such that b=λυ in similar to c=λυ for waves Other non-relativistic quantum equation are
derived for high speed charged particles such as p=mb ν=mbch λ=hmb E=hbλ E=mb2 and E=mbc
We believe that this b constant is of similar importance in non- relativistic quantum mechanics to
Planck constant h
Acknowledgement The author is highly indebted to Professor Dr G A W Derwish BSc PhD CChem FRSC for his
valuable and fruitful discussions suggestion and comments
References [1] Abraham M 1903 Ann d Phys vol 10 pp105 vol 14 pp236 1904
[2] Arthur D 1993 ldquoAntoine Lavoisier Science Administration and Revolutionrdquo Cambridge
University Press
[3] Arygres P 2001 ldquoAn Introduction to Global Supersymmetryrdquo
[4] Baer H and T Xerxes 2006 ldquoWeak Scale Supersymmetryrdquo Cambridge University Press
[5] Bakhoum E G 2002 Physics Essays 15 1 (Preprint archive physics0206061)
[6] Bartocci U Albert Einstein e Olinto De Pretto 1999 ldquoLa vera storia della formula pi`u famosa
del mondordquo (Ed Andromeda Bologna)
[7] Boltzmann L 1877 Proceedings of imperial Academy of Science Vienna (II) 76 pp 428
[8] Bohr N 1913 ldquoOn the Constitution of Atoms and Moleculesrdquo Philosophical Magazine
Series 6 26 pp 1-25
[9] Bromley D A 2000 ldquoGauge Theory of Weak Interactionsrdquo Springer ISBN 3-540-67672-4
[10] Clementi E and DL Raimondi 1963 J Chem Phys 38 pp 2686
[11] Clementi E DL Raimondi and WP Reinhardt 1967 J Chem Phys 47 pp 1300
[12] Cohen A B 1971 ldquoConcepts of Nuclear Physicsrdquo McGraw-Hill Chap 4
[13] Compton Arthur H 1923 ldquoA Quantum Theory of the Scattering of X-Rays by Light
Elementsrdquo Physical Review
[14] Cooper F A Khare and U Sukhatme 1995 Supersymmetry in Quantum Mechanicsrdquo Phys
Rep 251 pp 267-85
[15] Davisson C1965 The Discovery of Electron Waves Nobel Lectures Physics 1922-1941
Amsterdam Elsevier Publishing Company Retrieved on 2007-09-17
[16] Davisson C1937 Nobel Foundation The Nobel Prize in Physics 1937 Les Prix Nobel
Retrieved on 2007-09-17
[17] Drees M 1996 ldquoAn Introduction to Supersymmetryrdquo
[18] De Broglie L 1924 ldquoRecherches sur la theacuteorie des quantardquo (Researches on the quantum
theory) Thesis Paris
[19] Dugne J-J Fredriksson S and Hansson J Preon Trinity 2002 ldquoA Schematic Model of
Leptons Quarks and Heavy Vector Bosonsrdquo Europhys Lett 57 pp 188
[20] Eidelman S et al 2004 ldquoParticle data group the quark modelrdquo Physics Letters
B 592 pp 1
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
600 Bahjat R J Muhyedeen
[21] Einstein A 1905 Annalen der Physik 18 pp 639
[22] Encyclopedia Britannica 2008 Grand unified theory (GUT) Ultimate Reference
Suite Chicago Encyclopedia Britannica
[23] Fernbach S R Serber and TB Tayler 1949 ldquoThe Scattering of High-Energy
[24] Neutrons by Nucleirdquo Phys Rev 75 pp1352
[25] Freedman R and HYoung 2004 ldquoUniversity Physics with Modern Physicsrdquo
11th international edition Sears and Zemansky 1633-4 ISBN 0-8053-8768-4
[26] Freund P G O 1986 ldquoIntroduction to Supersymmetryrdquo Cambridge University Press
[27] Georgi H ldquoLie algebras in particle physicsrdquo Addison-Wesley Longman
ISBN 0-7382-0233-9
[28] Glashow SL 1961 Partial-symmetries of weak interactions Nuclear Physics 22(4) 579ndash
588
[29] Goodman J W 1996 ldquoIntroduction to Fourier opticsrdquo New York McGraw-Hill ISBN 0-07-
024254-2
[30] Hambsch FJ et al 1989 Nucl Phys A 491 pp 56
[31] Hasenoumlhrl F 1904 Ann d Phys vol 15 pp344
[32] Hawking S 1988 ldquoA Brief History of Timerdquo
[33] Hertz HR1887 May Ueber sehr schnelle electrische Schwingingungen Annalen der
Physik2 31 pp 421
[34] Hertz HR1888 March Ueber Einwirkung einer geradlinigen electrische Schwingingung
Annalen der Physik 2 34 pp 155
[35] Hertz HR1888 May Ueber Ausbreitungsgeschwindigkeit der electrodynamische Annalen
der Physik 2 34 pp 551
[36] Heisenberg W 1927 Uumlber den anschaulichen Inhalt der quantentheoretischen
Kinematik und Mechanik Zeitschrift fuumlr Physik 43 pp 172-198
[37] Junker G 1996 ldquoSupersymmetric Methods in Quantum and Statistical Physicsrdquo Springer-
Verlag
[38] Kane G L 1987 ldquoModern Elementary Particle Physicsrdquo Perseus Books ISBN 0-201-11749-
5
[39] Kaufmann W 1902 Phys Z vol 4 pp 55
[40] Lawson J D 1957 Proceedings of the Physical Society B Vol 70 pp 6
[41] Leibniz G W 1717 ldquoPhilosophical Essaysrdquo Ed and trans by Roger Ariew and Daniel
Garber Indianapolis Hackett 1989 Indianapolis Indiana 46204
[42] Lykken J D 1996 ldquoIntroduction to Supersymmetryrdquo
[43] Mackie J M 1845 The Life of Godfrey William von Leibnitzrdquo Written by G E Guhrauer
in 1809-1854 Full text PDF trans by Mackie Boston USA
[44] Martin S 1999 ldquoA Supersymmetry Primerrdquo
[45] Maxwell J M 1861 ldquoOn Physical Lines of Forcerdquo
[46] Maxwell J M 1865 ldquoA Dynamical Theory of the Electromagnetic Fieldrdquo
[47] Mehra J and H Rechenberg 1982 The Historical Development of Quantum Theory
Volume 1 Chapter 1 Springer
[48] Muhyedeen B R J A T Al- Thib and G A W Derwish 1993 Iraqi J Chem 11 3
[49] Newton I 1704 ldquoOpticksrdquo pp CVX (reprinted by Dover Publications Inc New York
(1952)
[50] Newton I 1726 ldquoThe Principia Mathematical Principles of Natural Philosophyrdquo (Trans I B
Cohen and A Whitman) Berkeley CA University of California Press 1999
[51] Ohrl H and Wien F Sitzungen 1904 F Ann der Phys IIA 113 pp 1039 Ohrl H 1905 F
Ann der Phys 16 pp 589
[52] Oberst H D Kouznetsov K Shimizu J Fujita F Shimizu 2005 ldquoFresnel diffraction mirror
for atomic waverdquo Physical Review Letters 94 pp 013203
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005
On a Heuristic Viewpoints Concerning the Mass Energy and Light Concepts in Quantum Physics 601
[53] Parker B 1993 ldquoOvercoming some of the problemsrdquo pp 259-279
[54] Pati J C and A Salam 1974 ldquoLepton number as the fourth color Phys Rev D10 pp 275-
289
[55] Planck M 1901 rdquoOn the Law of Distribution of Energy in the Normal Spectrumrdquo Annalen der
Physik 4 pp 553
[56] Planck M 1908 Ann Phys 26 pp 1
[57] Planck M 1907 Sitz der preuss AkadWiss Physik Math Klasse 13 (June)
[58] Poincaracutee JH 1900 Arch neerland sci 2 5 pp 232
[59] Poincaracutee JH 1900 In Boscha pp 252
[60] Preston S T 1875 ldquoPhysics of the Etherrdquo E amp F N Spon London see also
httpitisvoltaalessandriaitepistemeep6ep6-bjerk1htm
[61] Pretto O De 1904 ldquoIpotesi dellrsquoetere nella vita dellrsquouniversordquo Reale Istituto Veneto di
Scienze Lettere ed Arti Feb 1904 tomo LXIII parte II pp 439-500
[62] Rohlf J W 1994 ldquoModern Physics from a to Z0rdquo Wiley
[63] Rutherford E 1904 ldquo Radio-activity 2nd ed (1905) ISBN 978-1-60355-058-1
[64] Rutherford E 1906 ldquoRadioactive Transformationsrdquo ISBN 978-160355-054-3
[65] Rutherford E 1904 ldquoRadiations from Radioactive Substancesrdquo
[66] Rutherford E 1926 ldquoThe Electrical Structure of Matterrdquo
[67] Rutherford E 1933 ldquoThe Artificial Transmutation of the Elementsrdquo
[68] Schroumldinger E 1926 An Undulatory Theory of the Mechanics of Atoms and Molecules
Phys Rev 28 6 pp 1049ndash1070 doi101103 Phys Rev 28 pp 1049
[69] Schroumldinger E 1926 Annalen der Physik (Leipzig) Main paper
[70] Schwarz P 1998 ldquoThe Official String Theory Web Siterdquo Retrieved on December 16 2005
March 2008
[71] Singer C 1941 ldquoA Short History of Science to the Nineteenth Century Clarendon Press pp
217
[72] Soddy F 1904 ldquoRadioactivity An Elementary Treatise from Standpoint of the Disintegration
Theoryrdquo (ldquoThe Electrician ldquoPrinting and Publishing London)
[73] Slater J C 1960 ldquoQuantum Theory of Atomic Structure Volumes I amp II McGraw-Hill NY
[74] Straede C et al 1987 Nucl Phys A 462 pp 85
[75] Thiereus H et al 1981 Phys Rev C 23 pp 2104
[76] Troost J 2002 ldquoBeyond String Theoryrdquo Vrije Universiteit Brussel Theoretical Physics
(TENA) Retrieved on December 16 2005 ndash An ongoing project by a string physicist working
for the French CNRS
[77] Weinberg S 1967 A Model of Leptons Physical Review Letters 19 (21) 1264ndash1266
[78] Wilkins B D et al 1976 Phys Rev C 14 pp1832
[79] Witten E 1998 ldquoDuality Spacetime and Quantum Mechanicsrdquo Kavli Institute for Theoretical
Physics Retrieved on December 16 2005