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Introduction | ||
1 | Phase Space Model of Particle Production | 1 |
1.1 | High energy nuclear events | 6 |
1.2 | On multiparticle production in a single interaction process | 20 |
1.3 | Statistical thermodynamics of strong interactions at high energies | 24 |
1.4 | On the hadronic mass spectrum | 64 |
1.5 | Strange anti-baryons from quark-gluon plasma | 69 |
2 | Perturbative QCD Plasma | 77 |
2.1 | Superdense matter: neutrons or asymptotically free quarks? | 77 |
2.2 | Fermions and gauge vector mesons at finite temperature and density. III. The ground-state energy of a relativistic quark gas | 86 |
2.3 | Theory of hadron plasma | 103 |
2.4 | Quantum chromodynamics at high temperature | 111 |
2.5 | Infrared problem in the thermodynamics of the Yang-Mills gas | 149 |
2.6 | Covariant calculations at finite temperature: the relativistic plasma | 153 |
2.7 | Spectrum of elementary Fermi excitations in quark-gluon plasma | 167 |
2.8 | Soft amplitudes in hot gauge theories: a general analysis | 169 |
3 | Lattice Gauge Theory | 235 |
3.1 | Lattice models of quark confinement at high temperature | 239 |
3.2 | Quark liberation at high temperature: a Monte Carlo study of SU(2) gauge theory | 248 |
3.3 | Monte Carlo study of SU(2) gauge theory at finite temperature | 248 |
3.4 | The order of the deconfinement transition in SU(3) Yang-Mills theory | 265 |
3.5 | On the existence of a phase transition for QCD with three light quarks | 269 |
3.6 | Remarks on the chiral phase transition in chromodynamics | 273 |
4 | Fluid Dynamics and Flow | 277 |
4.1 | On multiple production of particles during collisions of fast particles | 283 |
4.2 | Highly relativistic nucleus-nucleus collisions: The central rapidity region | 300 |
4.3 | Hydrodynamics of ultra-relativistic heavy ion collisions | 312 |
4.4 | Single particle distribution in the hydrodynamic and statistical thermodynamic models of multiparticle production | 342 |
4.5 | Evidence for a blast wave from compressed nuclear matter | 346 |
4.6 | Transverse momentum analysis of collective motion in relativistic nuclear collisions | 350 |
4.7 | Anisotropy as a signature of transverse collective flow | 355 |
5 | Strangeness | 372 |
5.1 | Strangeness production in the quark-gluon plasma | 378 |
5.2 | Quarkochemistry in relativistic heavy-ion collisions | 383 |
5.3 | How much strangeness production is there in ultrarelativistic nucleus-nucleus collisions? | 388 |
5.4 | Time evolution of strange-particle densities in hot hadronic matter | 398 |
5.5 | Separation of strangeness from antistrangeness in the phase transition from quark to hadron matter: possible formation of strange quark matter in heavy-ion collisions | 412 |
6 | Charm | 416 |
6.1 | J/[Psi] suppression by quark-gluon plasma formation | 419 |
6.2 | Color screening and deconfinement for bound states of heavy quarks | 426 |
7 | Electromagnetic Signals | 432 |
7.1 | Direct production of photons and dileptons in thermodynamical models of multiple hadron production | 436 |
7.2 | Quark-gluon plasma and the production of leptons, photons and psions in hadron collisions | 457 |
7.3 | Muon pair production in very high energy nucleus-nucleus collisions | 465 |
7.4 | Direct lepton production in high-energy collisions of nuclei | 471 |
7.5 | Dilepton emission and the QCD phase transition in ultrarelativistic nuclear collisions | 478 |
7.6 | High-energy photons from quark-gluon plasma versus hot hadronic gas | 487 |
8 | Quark-Gluon Plasma Formation | 503 |
8.1 | Minijet production in high-energy nucleus-nucleus collisions | 508 |
8.2 | The early stage of ultra-relativistic heavy ion collisions | 512 |
8.3 | Quark and gluon production in high-energy nucleus-nucleus collisions | 526 |
8.4 | HIJING: A Monte Carlo model for multiple jet production in pp. pA and AA collisions | 542 |
8.5 | Dynamics of parton cascades in highly relativistic nuclear collisions | 558 |
8.6 | Kinetic theory for plasmas with non-abelian interactions | 613 |
9 | Parton Energy Loss | 617 |
9.1 | Jets as a probe of quark-gluon plasmas | 620 |
9.2 | Jets in expanding quark-gluon plasmas | 626 |
9.3 | Gluon shadowing and jet quenching in A+A collisions at [actual symbol not reproducible] = 200A GeV | 633 |
10 | Density Interferometry | 637 |
10.1 | Influence of Bose-Einstein statistics on the antiproton-proton annihilation process | 641 |
10.2 | Like particle correlations as a tool to study the multiple production mechanism | 654 |
10.3 | Pion interferometry of nuclear collisions. I. Theory | 657 |
10.4 | Proton pictures of high-energy nuclear collisions | 683 |
10.5 | Pion interferometry for exploding sources | 688 |
10.6 | Pion interferometry of quark-gluon plasma | 691 |
11 | Disoriented Chiral Condensate | 705 |
11.1 | Classical states of the chiral field and nuclear collisions at very high energy | 708 |
11.2 | Soft-pion emission in high-energy heavy-ion collisions | 712 |
11.3 | Static and dynamic critical phenomena at a second order QCD phase transition | 718 |
12 | Phase Transition Dynamics and Cosmology | 749 |
12.1 | Cosmic separation of phases | 752 |
12.2 | Big bang nucleosynthesis and the quark-hadron transition | 766 |
12.3 | Bubble growth and droplet decay in the quark-hadron phase transition in the early Universe | 771 |
12.4 | Dynamics of the QCD phase transition | 791 |
13 | Color Superconductivity | 795 |
13.1 | Superconducting quark matter | 798 |
13.2 | Superconductivity in quark matter | 802 |
Author Index | 817 |
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