we claim – in our system all states are localized. why?
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e. x. We claim – in our system all states are localized. Why?. Few General Concepts. The physical scene we would be interested in. Creating electronic continuity. Wave-functions of first confined states ( probability to find electron at z = z 0 ) - PowerPoint PPT PresentationTRANSCRIPT
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We claim – in our system all states are localized. Why?
x
e
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Few General Concepts
The physical scene we would be interested in
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Z
Creating electronic continuity
E
E1
P
0
Wave-functions of first confined states( probability to find electron at z = z0)( Energy level of the state )
Spatial proximity leads to wave-function overlap.
E11
E12
E1 E1
E11
E12
(a) (b)
(c)
The distance determines the strength of the overlap or DE=E12-E11.
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E1 E1*
E11
E12
E1E1
*
E11
E12
E1
E1*
E11
E12
E1
E1*
E11
E12
Two states are equally shared by the sites
Two states are separate
(Two identical pendulum in resonance)
(Very different pendulum do not resonate - stronger disorder)
Strong coupling overcomes minute differences (low disorder)
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E0E0 E0+r1
E0 E0+
r2
E0
E0 E0+r1
E0 E0+
r2
+
r3
+E1
E2
E3
E4No long range “resonance”
Lifshitz Localization
If there is a large disorder in the spatial coordinates no band is formed and the states are localized.
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Conjugation length Long Short
Varying chain distance
Strong coupling Weak coupling
Coupling also affected by relative alignment of the chains (dipole)
parallel shift tilt
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Localization in “Soft” matter
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Polymers: carbon based long repeating molecules-conjugation: double bond conjugation
What are conjugated polymers?
MEH-PPVpoly[acetylene]
Molecular organicSemiconductor
CC
H
H
CC
H
H
CC
H
H
CC
H
H
CC
H
H
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Conjugation
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sp2sp2
sp2
sp2
sp2
sp2
sp2sp2
sp2
sp2
electrons delocalised
electrons localised
sp2sp2
sp2
sp2
sp2
sp2
sp2sp2
sp2
sp2
sp2
sp2
sp2sp2
sp2
sp2
electrons delocalised
electrons localised
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+ +--
p-
p+
p-
p+
Bonding
=
p-
p+
p+
p- + +--Anti-bonding
*=
Z
Amplitude
p+
p-
The phase of thewave function
Molecular levels
Stable state
Less Stable state
Consider 2 atoms
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4 atoms
HOMO(Valence)
LUMO(Conduction)
There is correlation between spatial coordinates and the electronic configuration!!
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atoms4
HOMO(Valence)
LUMO(Conduction)
Molecule’s Length
Energy
atoms4
HOMO(Valence)
LUMO(Conduction) atoms4
HOMO(Valence)
LUMO(Conduction)
atoms4
HOMO(Valence)
LUMO(Conduction)
atoms4
HOMO(Valence)
LUMO(Conduction)
Configuration coordinate
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cc
cc
cc
cc
cc
Sigma
Dimerised (1)
Dimerised (2)
(a)
(b)
(c)
(d)
) b(
) c( ) d(
Ener
gy
) b(
) c( ) d(
Ener
gy
Bond Length
Degenerate ground state
Another coordinate system
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Aromatic link
Quinoidal link
General or schematic configuration coordinate
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The potential at the bottom of the well is ~parabolic (spring like)
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Q0
E0spring
E=E0+B(Q-Q0)2
Spring Energy
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-2000
0
2000
4000
6000
8000
1 104
1.2 104
-40 -20 0 20 40
E
Q
Elastic energy:2
elastE BQ
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
Equilibrium
Stretched
Squeezedc
cc
cc
cc
cc
cc
cc
cc
cc
cc
c
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
cc
2elastE BQ
Simplistic approach
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Q0
E0t= E0spring+E0elec Q
Here, the particle just entered the system (molecule) and we see the state before the environment responded to its presence (prior to relaxation)
The system relaxed to a new equilibrium state. In the process there was an increase in elastic energy of the environment and the electron’s energy went down. On the overall energy was released (typically) as heat.
Adding a particle will raise the system’s energy by (m*g*h)
On a 2D surface
The particle dug himself a hole (self localization)
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Q0
E0spring
Q
-1000
0
1000
2000
3000
4000
5000
6000
-30 -20 -10 0 10 20 30 40
E
Q
A
A*
A A*
If the potential energy of the mass would not depend on its vertical position
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Q
-1000
0
1000
2000
3000
4000
5000
6000
-30 -20 -10 0 10 20 30 40
E
Q
A*
A*
If the potential energy of the mass would not depend on its vertical position
A’
We’ll be interested in the phenomena arising from the relation between the length of the spring and the particle’s potential energy.
We’ll claim that due to this phenomenon there the system (electron) will be stabilized
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2 22
22ne
E nm L
2 22
322n
edE n dL F dL
m L
L L + dL
Stretch modeEn
En +dEn
For small variations in the “size” of the molecule the electron phonon contribution to the energy of the electron is linear with the displacement of the molecular coordinates.
For -conjugated the atomic displacement is ~0.1A and F=2-3eV/A.
The general formalism: Ee-ph=-AQ
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Linear electron-phonon interaction:
e phE AQ
0
20
elast e phE E E E
E E BQ AQ
2 22min min 2 2 4b
A A AE BQ AQ B AB B B
The system was stabilized by DE through electron-phonon interaction Polaron binding energy
0EQ
0 0 _ 0 _ 0 _ ; elast e e nE E E E E
-1000
0
1000
2000
3000
4000
5000
6000
-30 -20 -10 0 10 20 30 40
E
Q
bE
minQ
0 elast e phE E E E 0 elastE E E
min 2AQB
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0
500
1000
1500
2000
2500
3000
-20 -10 0 10 20 30
E
Q2
Molecule without e-ph relaxation
0
500
1000
1500
2000
2500
3000
-20 -10 0 10 20 30
E
Q1
Molecule with e-ph relaxation
minQWhat is the energy change, at Qmin, due to reorganization?
“stretch” the molecule to the configuration associated with the e-ph relaxation and see how much is gained by the e-ph relaxation.
2min 2b bBQ E E
0
500
1000
1500
2000
2500
3000
-20 -10 0 10 20 30
E
Q1
What is ?
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Why all this is relevant to charge transport?
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-20 -10 0 10 20 30
E
Q2
Molecule without a charge
-20 -10 0 10 20 30
E-E
0_E
lect
Q1
Molecule containing a charge
If the two molecules are identical and have the same E0 The electron carries En+AQ1 and replace it with En+AQ2 Transfer is most likely to occur when Q1=Q2=Q
Total excess energy to reach this state: 2 2minW B Q Q BQ
Transfer will occur when by moving the electron from one molecule to other there would be no change in total energy.
minQ
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Transfer will occur when Q1=Q2=Q
Total excess energy to reach this state: 2 2minW B Q Q BQ
2 2min min
102MinW B Q Q BQ Q Q
Q
22min
1 1 12 2 4 2a Min b
AW W BQ EB
200aW meV
Electron transfer is thermally activated process /aW
kT qe
Typical number is:
To move an electron or activate the transport we need energy of:
min 2AQB
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E
Q
E
EC
Polaron Binding Energy
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So far we looked into:
A A*
Let’s look at the entire transport reaction:
A + D* A* + D
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E
Q1
E
Q2
E
Q*
Two separate molecules
One reaction or system
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0
2000
4000
6000
8000
1 104
-40 -20 0 20 40
E
Q*
A system that is made of two identical molecules
As the molecules are identical it will be symmetric (the state where charge is on molecule A is equivalent to the state where charge is on molecule D)
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E
Wa
4Wa=2Eb
If the reactants and the products have the same parabolic approximation:
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-1000
0
1000
2000
3000
4000
5000
6000
E
Q*
A system that is made of two identical molecules
As the molecules are identical it will be symmetric (charge on A is equivalent to charge on D)
Wa
D A D A
Reactants Products
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AqWkT
phononR e P
Average attempt frequency Activation of the
molecular conformation
Probability of electron to move (tunnel) between two “similar” molecules
Requires the “presence” of phonons.Or the occupation of the relevant phonons should be significant
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What is a Phonon? Considering the regular lattice of atoms in a uniform solid material, you would expect there to be energy associated with the vibrations of these atoms. But they are tied together with bonds, so they can't vibrate independently. The vibrations take the form of collective modes which propagate through the material. Such propagating lattice vibrations can be considered to be sound waves, and their propagation speed is the speed of sound in the material. The vibrational energies of molecules, e.g., a diatomic molecule, are quantized and treated as quantum harmonic oscillators. Quantum harmonic oscillators have equally spaced energy levels with separation DE = hu. So the oscillators can accept or lose energy only in discrete units of energy hu. The evidence on the behavior of vibrational energy in periodic solids is that the collective vibrational modes can accept energy only in discrete amounts, and these quanta of energy have been labeled "phonons". Like the photons of electromagnetic energy, they obey Bose-Einstein statistics.
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Considering a “regular” solid which is a periodic array of mass points, there are “simple” constraints imposed by the structure on the vibrational modes.Such finite size (L) lattice creates a square-well potential with discrete modes.
Associating a phonon energy
vs is the speed of sound in the solid
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ConfigurationCo-ordinate
Ener
gy
01
2
01
2
ConfigurationCo-ordinate
Ener
gy
Q Q
For a complex molecule with many degrees of freedom we use the configuration co-ordinate notation:
phonon phononE h
For the molecule to reach larger Q – higher energy phonons states should be populated
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Bosons: 1 1( )1 1
Bose Einstein E hkT kT
f Ee e
What will happen if T<Tphonon/2
-1000
0
1000
2000
3000
4000
5000
6000
E
Q
-1000
0
1000
2000
3000
4000
5000
6000
E
Q
Wa
A B A B
Reactants Products
In the context of:
1 1( )11
effective phononeffective h TkT T
f hee
The relevance to our average attempt frequency:
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-1000
0
1000
2000
3000
4000
5000
6000
E
Q
A system that is made of two identical molecules
At low temperature the probability to acquire enough energy to bring the two molecules to the top of the barrier is VERY low.In this case the electron may be exchanged at “non-ideal” configuration of the atoms or in other words there would be tunneling in the atoms configuration (atoms tunnel!).[D. Emin, "Phonon-Assisted Jump Rate in Noncrystalline Solids," Physical Review Letters, vol. 32, pp. 303-307, 1974].
Wa
A B A B
Would the electron transfer rate still follow exp(-qWa/kT)
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High T regime:13 phononkT h ~200k in polymers
Activation energy decreases with Temperature
[N. Tessler, Y. Preezant, N. Rappaport, and Y. Roichman, "Charge Transport in Disordered Organic Materials and Its Relevance to Thin-Film Devices: A Tutorial Review," Advanced Materials, vol. 21, pp. 2741-2761, Jul 2009.]
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Are we interested in identical molecules?
(same A, B & E0)
x
e
Consider variations in E0
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E
DG1
DG0
qR qPqc
2R RV B q q
20P PV B q q G D
0 12 2
p Rc
p R
q qGqB q q D
Effect of disorder or applied electric field on the two molecule system:
2R PB q q
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21
20
20
2
2202
2020
12 2
2 2 228
2
8
1 14 4
c R
p RR
p R
p Rp R p R R
p R
p R
p R
G B q q
q qG qB q q
q qG B q q B q q q
B q q
G B q qB q q
GG
D
D
D
D
D D
B
For polaron transfer 2|Eb|) :21 01 2
8 bb
G G EE
D D
Energy activation for going to the lower site: 1GD
201 1
4
GG
D D
In the present case for going down in energy
201 1
2 2b
b
GEG
E
D D
In the present case for going down in energy
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2021 0
200
1 2 18 2 2
2 2 8
bb
b b
b
b
E GG G EE E
GE GE
D D D
DD
Energy activation for going to the lower site:
2
exp exp2 2 8
j i j ibi j i j
b
ER PkT kT kTE
e e e eu
This term is usually negligible
14j i
bE
e e
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E
DG1
DG0=Ei-Ej
qi qjqc
Effect of disorder or applied electric field on the two molecule system:
2
exp exp2 2 8
j i j ibi j i j
b
ER PkT kT kTE
e e e eu
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Gaussian Distribution of StatesE
1017cm-31018cm-3
Let’s consider a system characterized by:
x
e
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Detailed Equilibrium 1 1i j ij j i jif E f E f E f Eu u
exp j iij
ji kT
e euu
, 1 1 exp /i if E E kT
exp /
1 j i j i
ij j it
E E kT E EE E
elseu u
0
exp / exp
1 j i j i
ij
E E kT E E
elseu u
ijR
Another form:
P- V. Ambegaokar, B. I. Halperin, and J. S. Langer, "Hopping Conductivity in Disordered Systems," Phys. Rev. B,
vol. 4, pp. 2612-&, 1971.- A. Miller and E. Abrahams, "Impurity Conduction at Low Concentrations," Phys. Rev., vol. 120, pp. 745-755,
1960.
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hhhhh ndxdDEnJ
Under which circumstances can we use:
1 and D are statistical quantitiesA. Statistics has to be well definedB. Variation in the structure/properties are slow
compared to the length scale we are interested in
Gaussian Distribution of StatesE
1017cm-31018cm-3
1. Density and spatial regime2. Carrier sampling DOS