Under‐saturation of quarks at early stages of relativistic nuclear collisions: The hot glue initial scenario and its observable signatures
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H. Stoecker | B. Sinha | S. Raha | P. Zhuang | I. Mishustin | K. Zhou | L. Csernai | Z. Xu | V. Vovchenko | J. Steinheimer | C. Greiner | T. Bir'o | S. Schramm | M. Gorenstein | F. Senzel | J. Struckmeier | L. Satarov | M. Panero | K. Gallmeister | M. Beitel
[1] H. Stoecker,et al. Glueballs amass at the RHIC and LHC! the early quarkless first-order phase transition at T = 270 MeV - From pure Yang-Mills glue plasma to Hagedorn glueball states , 2015, 1509.00160.
[2] T. Neuhaus,et al. Critical point and scale setting in SU(3) plasma: An update , 2015, 1503.05652.
[3] V. Greco,et al. Quarks production in the quark–gluon plasma created in relativistic heavy ion collisions , 2015, 1502.04596.
[4] J. Uphoff,et al. Elliptic flow and nuclear modification factor in ultrarelativistic heavy-ion collisions within a partonic transport model. , 2014, Physical review letters.
[5] A. Monnai. Thermal photon v 2 with slow quark chemical equilibration , 2014, 1403.4225.
[6] C. Greiner,et al. Thermalization of Hadrons via Hagedorn States , 2014, 1402.1458.
[7] Fuming Liu,et al. Quark-gluon plasma formation time and direct photons from heavy ion collisions , 2012, 1212.6587.
[8] T. B. Skaali,et al. Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at root s(NN)=2.76 TeV , 2013, 1304.0347.
[9] L. Mclerran,et al. Thermalization and Bose-Einstein Condensation in Overpopulated Glasma , 2012, 1210.6838.
[10] V. Greco,et al. Quark-to-gluon composition of the quark-gluon plasma in relativistic heavy-ion collisions , 2012, 1202.2262.
[11] Z. Fodor,et al. Precision SU(3) lattice thermodynamics for a large temperature range , 2012, 1204.6184.
[12] H. Stoecker,et al. Longitudinal fluid-dynamics for ultrarelativistic heavy-ion collisions , 2006, hep-ph/0606074.
[13] C. Greiner,et al. Thermalization of gluons in ultrarelativistic heavy ion collisions by including three-body interactions in a parton cascade , 2004, hep-ph/0406278.
[14] S. Rasanen,et al. Photon production from non-equilibrium QGP in heavy ion collisions , 2004, nucl-th/0403040.
[15] Niels Bohr Institute,et al. Collective deceleration of ultrarelativistic nuclei and creation of quark-gluon plasma. , 2001, Physical review letters.
[16] R. Choudhury,et al. Hard photon production from unsaturated quark–gluon plasma at two-loop level , 2001, hep-ph/0104134.
[17] F. Karsch. Lattice results on QCD thermodynamics , 2001, hep-ph/0103314.
[18] L. Csernai,et al. Initial state of ultrarelativistic heavy ion collisions , 2000, hep-ph/0010307.
[19] A. Krasnitz,et al. Initial gluon multiplicity in heavy-ion collisions. , 2000, Physical review letters.
[20] D. Rischke,et al. Chemical equilibration of quarks and gluons at RHIC and LHC energies , 1999, nucl-th/9908004.
[21] P. Roy,et al. Quark Gluon Plasma Diagnostics in a Successive Equilibrium Scenario , 1997, nucl-th/9706034.
[22] K. Eskola,et al. Baryon-to-entropy ratio in very high energy nuclear collisions , 1996, nucl-th/9610015.
[23] Thoma,et al. Photon emission from a parton gas at chemical nonequilibrium. , 1995, Physical review. C, Nuclear physics.
[24] Alam,et al. Successive equilibration in quark-gluon plasma. , 1994, Physical review letters.
[25] R. Venugopalan,et al. Computing quark and gluon distribution functions for very large nuclei. , 1993, Physical review. D, Particles and fields.
[26] Biró,et al. Parton equilibration in relativistic heavy ion collisions. , 1993, Physical review. C, Nuclear physics.
[27] E. Shuryak,et al. Two-stage equilibration in high energy heavy ion collisions. , 1992, Physical review letters.
[28] M. Gyulassy,et al. HIGING: A Monte Carlo model for multiple jet production in pp, pA, and AA collisions. , 1991, Physical review. D, Particles and fields.
[29] Seibert,et al. High-energy photons from quark-gluon plasma versus hot hadronic gas. , 1991, Physical review. D, Particles and fields.
[30] B. Kämpfer,et al. Correlations between dilepton yields and pion multiplicities as probe of the deconfinement transition , 1990 .
[31] S. Raha. Dilepton, Diphoton and Photon Production in Preequilibrium , 1990 .
[32] Hwa,et al. Diagnosing quark matter by measuring the total entropy and the photon or dilepton emission rates. , 1985, Physical review. D, Particles and fields.
[33] E. Levin,et al. Semihard processes in QCD , 1983 .
[34] H. Satz,et al. The latent heat of deconfinement in SU(3) Yang-Mills theory , 1983 .
[35] H. Satz,et al. THE ORDER OF THE DECONFINEMENT TRANSITION IN SU(3) YANG-MILLS THEORY , 1983 .
[36] James D. Bjorken,et al. Highly Relativistic Nucleus-Nucleus Collisions: The Central Rapidity Region , 1983 .
[37] L. Hove,et al. High-energy hadron-hadron collisions and internal hadron structure , 1975 .