1. Dynamic Time Scales in Colored Glass Nuclear Matter
Vivek Parihar
A. Widom
Y. N. Srivastava
NORTHEASTERN UNIVERSITY, BOSTON,
UNIV.of PERUGIA & INFN, ITALY
ISSP ‘06

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3. VIVEK PARIHAR

4. hydrodynamic expansion
initial state
pre-equilibrium
QGP and
hydrodynamic expansion
hadronization
hadronic phase
and freeze-out
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5. Quarks and String Glass
QED Vacuum
QCD Vacuum
Quark Potential and String Tension
Rotating Strings
Entropy of String Configurations
Relaxation Time Scales
Glass Laws
High Energy Nuclear Scattering
Conclusions
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6. Quantum Electrodynamic Vacuum Instability I
Static Dielectric Screening of Coulomb’s Law at Short Distance
Dynamic Conductivity s(w) of the Dissipative Vacuum
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7. Quantum Electrodynamic Vacuum Instability II
Dissipative Vacuum Conductivity Yields a Landau Vacuum Ghost Instability at a Space-Like Wave Vector K
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8. Quantum Chromodynamic Vacuum Instability I
Vacuum Fluctuations Derek B. Leinweber
Dynamic Color Conductivity Re ss(w) < 0 Implies an “Amplifying Vacuum”
Since es(Q2) > 0 is always true, there are no Landau QCD ghosts.
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9. Quantum Chromodynamic Vacuum Instability II
Quark Potential
Linear Potential and String Tension s
Amplifying Vacuum Screening
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10. Bohr-Landau-Fermi Liquid Droplet Model of Nuclear Matter
Spherical Droplet Radius
Nucleons are in reality relativistic constituents of nuclei. The non-relativistic “shell model” must thereby be “patched up” by a strong LS- coupling for “simulating relativity”.
Fermi Velocity R
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11. Quark-Anti-Quark Pairs Color Electric Flux Tube
Quark-String Model I
Quark
Baryon Number
A=3(Nu+Nd)
Charge
Z=(2Nu+Nd)
N=(2Nd+Nu)
Mesons
Quark-Anti-Quark Pairs
Color Electric Flux Tube
“String”
s = gEcolor
Anti-Quark
A=Z+N
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12. Quantum String “Trajectory” Experimental Tension s
Quark-String Model II
Rotating String c -R R -c
Quantum String “Trajectory”
Experimental Tension s
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13. Quark-String Model III
Rotating and Vibrating Strings
(Mesons)
Entropy S(E) = kB ln W(N)
Hardy-Ramanujan Formula
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14. Entropy of Rotating and Vibrating Strings
Quark-String Model IV
Entropy of Rotating and Vibrating Strings
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15. Quark-String Model V F = (7/2)kBTH Relaxation Times Obey the Glass Law
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16. String Fragmentation Model for Quark Pairs on Strings
Quark-String Model VI m
String Fragmentation Model for Quark Pairs on Strings m s m s m s m m
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17. High Energy Scattering I
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18. High Energy Scattering II
Impact Parameter Representation b=l/k
Inelastic Scattering Dominates Elastic Scattering as E Becomes Very Large and
sel << sin
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19. High Energy Scattering III
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20. High Energy Scattering IV
Nuclear Target String State
Final Fragments with Constant Heat Capacity C
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21. Conclusion and Discussion
QED Vacuum has been Compared with QCD Vacuum
QCD Inspired “String Model”
Glass-Like Entropy of String Configurations
High Energy Nuclear Scattering Cross Sections
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