01/22/2009 francis marion university 1 the little big bang: relativistic nuclear collisions and the...
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01/22/2009Francis Marion University
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The Little Big Bang: Relativistic Nuclear Collisions and the Physics at 1012 KNathan Grau
Columbia University, Nevis Laboratories
01/22/2009Francis Marion University
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Outline Top-down introduction to high energy physics
and the Quark-Gluon Plasma The Quark-Gluon Plasma now
What we know now from the Relativistic Heavy Ion Collider (RHIC)
The Quark-Gluon Plasma in the future What we are learning and will learn from the
Large Hadron Collider, string theory, and trapping supercold atoms
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Introduction and Background of High Energy Physics
WARNING!The units you are about to see and hear are “natural”c = hbar = kB = 1Energy in GeV, momentum GeV/c (p~mc), mass in GeV/c2 (E=mc2)
Some important numbers to set a scale:Proton mass = 1 GeV/c2
170 MeV = 1012 K (E=kBT)
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The Standard Model Lagrangian This is the culmination of 400+ years of physics research All current physics data is
explained Disclaimer: Gravity Not
Included Still not small enough to fit
on a T-shirt Good party trick: Ask where
the sign error is (there really is one!)
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The Standard Model Condensed
The particles (fields) 12 particles 4 force carriers
Their interactions are the fundamental forces of nature…
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Fundamental Forces: Electroweak 1/2 Electroweak Force =
Electricity and Magnetism Everything from transistors in
computers to wind is governed by this force
Actually a single force: Electromagnetic force
Interaction of two charged entities
Theory: Quantum Electrodynamics (QED)
Computer Chip
Hurricane Katrina
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Fundamental Forces: Electroweak 1/2 Electroweak Force =
Weak Force interaction of two “weakly”
charged particles It is why the sun shines. In the first part of the chain the
proton turns into a neutron.
p p p p
He
light
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Fundamental Forces: Strong Force
g g
gproton
g
g g
neutron Quarks combine to form
other particles Baryons (qqq): protons,
neutrons, etc. Mesons( ): pions, kaons,
etc. Held together by gluons
Quark charge is “color” of 3 types: red, green, blue Contrast that with 2 electric
charges: +,- Hadrons are color neutral =
white
€
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Fundamental Forces: Strong Force
g g
gproton
g
g g
neutron Quarks combine to form
other particles Baryons (qqq): protons,
neutrons, etc. Mesons( ): pions, kaons,
etc. Held together by gluons
Quark charge is “color” of 3 types: red, green, blue Contrast that with 2 electric
charges: +,- Hadrons are color neutral =
white Theory: Quantum
Chromodynamics (QCD)
€
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Fundamental Forces: Strong Force
g g
gproton
g
g g
neutron
Ca. 1970 view of the proton and the neutron.Only real improvement is that the proton bubbles with lots of gluons and pairs
€
Quarks combine to form other particles Baryons (qqq): protons,
neutrons, etc. Mesons( ): pions, kaons,
etc. Held together by gluons
Quark charge is “color” of 3 types: red, green, blue Contrast that with 2 electric
charges: +,- Hadrons are color neutral =
white Theory: Quantum
Chromodynamics (QCD)
€
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Proton Structure
u
u
d
€
qq g
g
u
u
d
€
qq g
g
Proton at two instances in time The interior bubbles with pairs and gluons
€
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Proton Structure Probability of
finding a gluon or quark of a given flavor with momentum fraction x = pq/pp
u, d = valence near x~10-1
s,c,b,g = sea
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Fundamental Forces: Strong Force Strong force also binds nuclei Clearly needed another nuclear force since an
electrically neutral neutron could not bind with a positive proton via electromagnetic force
In fact, individual proton and
neutron definitions are
blurred by quantum
mechanics Nucleus is a bag of quarks and
gluons
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Confinement
Quarks and gluons are confined - no evidence of their existence outside of (colorless) hadrons
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The Quark-Gluon Plasma The state of the universe before it cooled to allow
hadrons (protons, neutrons, etc.) to form t < 1 s after the Big Bang
Hence part of my title T > 1012 K
Hence the other part of my title R < 1 fm = size of the proton
It is a different state of matter than what exists today Can we reproduce it in a laboratory?
Allow a direct study of the strong interaction which is 1/2 of the Standard Model.
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QCD Phase Diagram A beginning
definition: A hot, dense state of weakly-interacting quarks and gluons over a distance greater than the size of the proton.
Quark-Antiquark imbalance
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QCD Phase Diagram A beginning
definition: A hot, dense state of weakly-interacting quarks and gluons over a distance greater than the size of the proton.
Expected to occur at 1012K~170 MeV
Quark-Antiquark imbalance
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QCD Phase Diagram A beginning
definition: A hot, dense state of weakly-interacting quarks and gluons over a distance greater than the size of the proton.
Expected to occur at 1012K~170 MeV Heavy Ion Collision Trajectory
Quark-Antiquark imbalance
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The Relativistic Heavy Ion Collider (RHIC) From Space
NYCNYC
I live hereI live here
RHIC
At Brookhaven National
Laboratory
RHIC
At Brookhaven National
Laboratory
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RHIC Vitals and Statistics
• Two independent rings 3.83 km in circumference
– 120 bunches/ring
– 106 ns crossing time
• Maximum Energy
– s½ = 500 GeV p+p
– s½ = 200 GeV/N-N A+A
• Design Luminosity
– Au+Au 2x1026 cm-2s-1
– p+p 2x1032 cm-2s-1 ( polarized)
• Capable of colliding any nuclear species on any other nuclear species
• Collision energy = two mosquitoes colliding
• Collision temperature: over 1 trillion degrees
• Over 35,500 kg (78,100 pounds) of helium
• Ring cooled to 4.6 Kelvin (-450 degrees F)
• Refrigerator uses 15 MW electricity
• 20 years, less than one gram of gold is used
• Quark-gluon plasma lasts less than 0.00000000000000000000001 seconds
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A Relativistic Heavy Ion Collision Two nuclei approach
one another Moving at v=0.9995c so
relativistically contracted Mostly pass through
one another Overlap region
converts energy into heat and particles to form the QGP
Peripheral collision Not fully overlapping See “participants” and
“spectators”
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Simulations by the Frankfurt UrQMD Group
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A Relativistic Heavy Ion Collision
Central (head-on) Au+Au Collision
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Animation by Jeffery Mitchell (Brookhaven National Laboratory). Simulation by the UrQMD Collaboration
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Measuring
If is the quark-antiquark imbalance then measure anti-particle/particle ratios
Compare to a statistical model of hadronization
Note the species measured: K, K*, p,
M. Kaneta, N. Xu, nucl-th/0405068 (2004)
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Measuring M. Kaneta, N. Xu, nucl-th/0405068 (2004)
If is the quark-antiquark imbalance then measure anti-particle/particle ratios
Compare to a statistical model of hadronization
Note the species measured: K, K*, p,
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Measuring M. Kaneta, N. Xu, nucl-th/0405068 (2004)
B~30 MeV
If is the quark-antiquark imbalance then measure anti-particle/particle ratios
Compare to a statistical model of hadronization
Note the species measured: K, K*, p,
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Measuring T Look at the
photons Just like
COBE measures the CMB
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Measuring T: Photon Spectrum Yield of photons at
each momentum bin Dashed line is fit to
p+p data Extra photons in
Au+Au collisions exp(-pT/T) with
T = 221+/-23(stat.)+/-18(sys.) MeV
Other theoretical models are yield T from 300-600 MeV
Recall transition at T~170 MeV
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Measuring T: Photon Spectrum Yield of photons at
each momentum bin Dashed line is fit to
p+p data Extra photons in
Au+Au collisions exp(-pT/T) with
T = 221+/-23(stat.)+/-18(sys.) MeV
Other theoretical models are yield T from 300-600 MeV
Recall transition at T~170 MeV
Central Au+Au
Non-central Au+Au
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Measuring T: Photon Spectrum Yield of photons at
each momentum bin Dashed line is fit to
p+p data Extra photons in
Au+Au collisions exp(-pT/T) with
T = 221+/-23(stat.)+/-18(sys.) MeV
Other theoretical models are yield T from 300-600 MeV
Recall transition at T~170 MeV
Central Au+Au
Non-central Au+Au
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Intermediate Conclusion It seems like RHIC has indeed produced the
right conditions to produce a Quark-Gluon plasma.
But… Do we know it is thermalized? Is that temperature
from the photons really a temperature. What about other thermodynamic quantities:
pressure, entropy, etc.? Is there an equation of state?
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Getting at the Pressure: Elliptic Flow Non-overlapping
collisions of spherically symmetric nuclei results in a non-symetric overlap region Differential pressure
gradients if you think in terms of a fluid.
Use flow to measure Equation of State and speed of sound cs
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Azimuthal Distributions: v2
Particles have a harmonic distribution wrt the reaction plane.
v2 related to the strength of the modulation Dependent on
the particle’s momentum and mass
€
dN
dφ=
N
2π1+ 2v2 cos 2φ( ) + ...( )
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Compilation of Light Hadron v2 Data
Everything flows
Hydrodynamics fit data at low momentum Should not
work at high momentum
Can add K*, to this list as wellHydrodynamics = Fluid equations assuming
An equation of state and thermalization.
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v2 Scaling (I) With more
precise data scaling of baryons (p,n) and mesons (,K) observed.
€
KE T= mT − m = pT2 + m2 − m
baryons(qqq)
Mesons ( )
€
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v2 Scaling (II) Divide by the
constituent quarks and a universal v2 curve exists! nq=3 for
baryons nq=2 for
mesons Can be used
to derive a speed of sound: cs = 0.35+/-0.05
€
KE T= mT − m = pT2 + m2 − m
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Heavy Quarks Flow Also! Heavy
Flavor(HF): c,b e
c,b flow as well!
Like boulders flowing in a small stream
Several models ofheavy flavor diffusionthrough the medium
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Strongly Interacting Plasma
Hydrodynamic models work Only works with QGP equation of state (not a hadron gas) Implies local thermodynamic equilibrium Have viscosity = 0!
The medium produced is a perfect fluid Fluid! Not a gas! Heavy flavors are also strongly coupled to the fluid Data used to obtain (shear)viscosity/entropy density /s Light hadron v2 indicates /s ~ 1/4 Heavy hadron v2 indicate /s ~ (1-2)/4
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Should We Have Seen This Coming?
Lattic calculations (numerically solving QCD) indicate a phase transition
But new phase doesn’t reach the Stefan-Boltzmann limit The limit for non-
interacting paticles.
€
εQGP ≈ 34 εSB
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How Can We Make Headway? If particles are strongly coupled cannot use
perturbative methods to calculate Need a new tool that can calculate strongly
coupled field theories Why not use string theory????
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5-D Anti-de Sitter
Black Hole
5th dim
AdS/CFT Correspondence
Maldecena’s Conjecture 1) Calculate some
quantities in a 5-D gravity
Anti-de Sitter (AdS) defines the General Relativity metric
4-D
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AdS/CFT Correspondence Maldecena’s
Conjecture 2) Apply a
dictionary to get analogous quantity in the dual conformal field theory (CFT)
CFT: scale invariant field theory
QCD is not quite scale invariant Shh don’t tell…
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J. Maldacena
E. Witten
et al.
Black Hole
5th dim
5-D Anti-de Sitter
4-D
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AdS/CFT Correspondence
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QuickTime™ and aTIFF (LZW) decompressor
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J. Maldacena
E. Witten
et al.
r0~1/TQGP
4-DQCD-like,strongly-coupledfluid at TQGP
Black Hole
Conformalboundary
5th dim
5-D Anti-de Sitter
4-D
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What Do Strings Tell Us? Limit of /s (looks like an uncertainty
relationship)
Checked by many different geometries - seems universal!
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/s For Physical Substances
Nothing comes close to the physical bound except the QGP at TC
Recall Light hadron v2 indicates
/s~1/4 Heavy hadron v2 indicate
/s~(1-2)/4 Most perfect fluid ever
measured in a laboratory
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New Experiments: Large Hadron Collider (LHC) New, large,
higher-energy collider just turning on in CERN, Geneva Switzerland.
200 GeV Au+Au at RHIC to 5.5 TeV Pb+Pb at LHC
~100 m below
ground
27 km
5.5 TeV A+A14 TeV p+p
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ATLAS vs. RHIC Acceptance
Unprecedented coverage to measure HI Collisions and their properties.
RHIC
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The Last 10 Years
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The Last 10 Years
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The Last 10 Years
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The Last 10 Years
Physics Publications in Refereed Journals BRAHMS - 19 PHENIX - 76 PHOBOS - ??? website down :( STAR - 86
10s of technical papers 1 “White Paper” after 2003 run summarizing
physics Before the strongly-interacting QGP
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The Last 10 Years
A phase transition in our understanding of the Quark Gluon Plasma has occurred: it is a strongly-interacting, perfect fluid!
Insights to calculating non-perturbative QCD has come from String Theory!
New experiments and overlaps with other fields will help us learn more about the matter that dominates the visible universe.
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Fundamental Forces: Strong Force
g g
gproton
g
g g
neutron Quarks combine to form
other particles Baryons: protons,
neutrons, etc. Mesons: pions, kaons, etc. Held together by gluons
Quarks have “color” charge is of 3 types: red, green, blue Contrast that with 2 electric
charges: +,- Quarks are confined -
no evidence of their existence outside of hadrons
Ca. 1970 view of the proton and the neutron.Only real improvement is that the proton bubbles with lots of gluons and pairs
€
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The Collider From Inside a DetectorBeam View
dN/d ~ 600Head-on (central) Au+Au
STAR
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AdS/CFT : QCD Correspondence Maldecena’s conjecture String theory is equivalent to a conformal (scale-
invariant) field theory in a lower dimension without gravity
Further it has been argued that strongly coupled field theories can be described by weak string theories.
Implication: strongly coupled QCD can be calculated by a gravity dual Gravity = General Relativity in many dimensions Lots of work in 5-dimensional Anti-de Sitter (AdS) space -
this just defines the metric connected with QCD in 4-dimensions.