NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = E.Shuryak Found 92 matches. 2021DE29 Phys.Rev. C 104, 024908 (2021) Many-body forces and nucleon clustering near the QCD critical point
doi: 10.1103/PhysRevC.104.024908
2021DE31 Nucl.Phys. A1016, 122336 (2021) Nucleon clustering at kinetic freezeout of heavy-ion collisions via path-integral Monte Carlo
doi: 10.1016/j.nuclphysa.2021.122336
2020SH06 Phys.Rev. C 101, 034914 (2020) Baryon preclustering at the freeze-out of heavy-ion collisions and light-nuclei production
doi: 10.1103/PhysRevC.101.034914
2020SH25 Eur.Phys.J. A 56, 241 (2020) Light-nuclei production and search for the QCD critical point
doi: 10.1140/epja/s10050-020-00244-3
2019SH07 Nucl.Phys. A982, 831c (2019) Baryon Clustering at the critical line and near the hypothetical critical point
doi: 10.1016/j.nuclphysa.2018.12.006
2019SH29 Phys.Rev. C 100, 024903 (2019) Baryon clustering at the critical line and near the hypothetical critical point in heavy-ion collisions
doi: 10.1103/PhysRevC.100.024903
2017RA23 Nucl.Phys. A967, 868 (2017) An Effective Model of QCD Monopoles
doi: 10.1016/j.nuclphysa.2017.04.045
2016LA13 Nucl.Phys. A950, 110 (2016) Classical interactions of the instanton-dyons with antidyons
doi: 10.1016/j.nuclphysa.2016.03.013
2016LA23 Nucl.Phys. A956, 789 (2016) Recent progress in understanding gauge topology, confinement and chiral symmetry breaking
doi: 10.1016/j.nuclphysa.2016.01.067
2015HI05 Phys.Rev. C 91, 054915 (2015) Femtoscopic signature of strong radial flow in high-multiplicity pp collisions
doi: 10.1103/PhysRevC.91.054915
2015KA19 Phys.Rev. C 91, 054913 (2015) Collective flow in high-multiplicity proton-proton collisions
doi: 10.1103/PhysRevC.91.054913
2014BA25 Phys.Rev. C 90, 014905 (2014) G.Basar, D.E.Kharzeev, E.V.Shuryak Magneto-sonoluminescence and its signatures in photon and dilepton production in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.90.014905
2014KA32 Phys.Rev. C 90, 014901 (2014) Collective interaction of QCD strings and early stages of high-multiplicity pA collisions
doi: 10.1103/PhysRevC.90.014901
2014SH17 Nucl.Phys. A928, 138 (2014) On chiral symmetry breaking, topology and confinement
doi: 10.1016/j.nuclphysa.2014.03.006
2013SH20 Nucl.Phys. A904-905, 349c (2013) Shocks and sounds in Quark-Gluon Plasma
doi: 10.1016/j.nuclphysa.2013.02.021
2013SH42 Phys.Rev. C 88, 044915 (2013) High-multiplicity pp and pA collisions: Hydrodynamics at its edge
doi: 10.1103/PhysRevC.88.044915
2013SH44 Phys.Rev. C 88, 054903 (2013) Sound edge of the quenching jets
doi: 10.1103/PhysRevC.88.054903
2013SH48 Phys.Rev. C 88, 064905 (2013) Sounds of the QCD phase transition
doi: 10.1103/PhysRevC.88.064905
2012SH26 Phys.Rev. C 86, 024907 (2012) Shocks in quark-gluon plasmas
doi: 10.1103/PhysRevC.86.024907
2011LU18 Phys.Rev. C 84, 061901 (2011) Universal hydrodynamics and charged hadron multiplicity at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.84.061901
2011ST19 Phys.Rev. C 84, 034908 (2011) Fate of the initial state perturbations in heavy ion collisions. II. Glauber fluctuations and sounds
doi: 10.1103/PhysRevC.84.034908
2011ST22 Phys.Rev. C 84, 044912 (2011) Fate of the initial state perturbations in heavy ion collisions. III. The second act of hydrodynamics
doi: 10.1103/PhysRevC.84.044912
2010FA07 Phys.Rev. C 82, 014902 (2010) Lifetime of electric flux tubes near the QCD phase transition
doi: 10.1103/PhysRevC.82.014902
2010YO02 Phys.Rev. C 81, 034905 (2010) Recombinant charmonium in strongly coupled quark-gluon plasma
doi: 10.1103/PhysRevC.81.034905
2009LI18 Phys.Rev.Lett. 102, 202302 (2009) Angular Dependence of Jet Quenching Indicates Its Strong Enhancement near the QCD Phase Transition
doi: 10.1103/PhysRevLett.102.202302
2009SH44 Phys.Rev. C 80, 054908 (2009); Erratum Phys.Rev. C 80, 069902 (2009) Fate of the initial state perturbations in heavy ion collisions
doi: 10.1103/PhysRevC.80.054908
2009YO04 Phys.Rev. C 79, 034907 (2009) Charmonium in strongly coupled quark-gluon plasma
doi: 10.1103/PhysRevC.79.034907
2008LI24 Phys.Rev. C 77, 064905 (2008) Electric flux tube in a magnetic plasma
doi: 10.1103/PhysRevC.77.064905
2008LI43 Phys.Rev.Lett. 101, 162302 (2008) The Magnetic Component of Quark-Gluon Plasma is also a Liquid
doi: 10.1103/PhysRevLett.101.162302
2007FL03 Phys.Rev. C 76, 065206 (2007) Influence of meson widths on Yukawa-like potentials and lattice correlation functions
doi: 10.1103/PhysRevC.76.065206
2007LI29 Phys.Rev. C 75, 054907 (2007) Strongly coupled plasma with electric and magnetic charges
doi: 10.1103/PhysRevC.75.054907
2007LU12 Phys.Rev. C 76, 021901 (2007) How much entropy is produced in strongly coupled quark-gluon plasma (sQGP) by dissipative effects?
doi: 10.1103/PhysRevC.76.021901
2007SH02 J.Korean Phys.Soc. 50, 384 (2007) A Gravity Dual of RHIC Collisions
2007SH08 Nucl.Phys. A783, 39c (2007) Conical Flow from Quenched Jets in sQGP
doi: 10.1016/j.nuclphysa.2006.11.010
2007SH41 Phys.Rev. C 76, 047901 (2007) Origin of the "ridge" phenomenon induced by jets in heavy ion collisions
doi: 10.1103/PhysRevC.76.047901
2006CA40 Nucl.Phys. A774, 577 (2006) J.Casalderrey-Solana, E.V.Shuryak, D.Teaney Conical Flow induced by Quenched QCD Jets
doi: 10.1016/j.nuclphysa.2006.06.091
2006FL01 Europhys.Lett. 74, 813 (2006) Possible evidence for "dark radiation" from Big Bang Nucleosynthesis data
doi: 10.1209/epl/i2006-10031-y
2006GE14 Phys.Rev. C 74, 044908 (2006) B.A.Gelman, E.V.Shuryak, I.Zahed Classical strongly coupled quark-gluon plasma. I. Model and molecular dynamics simulations
doi: 10.1103/PhysRevC.74.044908
2006GE15 Phys.Rev. C 74, 044909 (2006) B.A.Gelman, E.V.Shuryak, I.Zahed Classical strongly coupled quark-gluon plasma. II. Screening and equation of state
doi: 10.1103/PhysRevC.74.044909
2006LI40 Nucl.Phys. A775, 224 (2006) Polymer chains and baryons in a strongly coupled quark-gluon plasma
doi: 10.1016/j.nuclphysa.2006.06.169
2006SH34 Nucl.Phys. A774, 387 (2006) Toward the theory of strongly coupled Quark-Gluon Plasma (sQGP)
doi: 10.1016/j.nuclphysa.2006.06.058
2005SH10 Nucl.Phys. A750, 64 (2005) What RHIC experiments and theory tell us about properties of quark-gluon plasma? NUCLEAR REACTIONS 197Au(197Au, X), E=high; analyzed data; deduced strongly coupled quark-gluon plasma.
doi: 10.1016/j.nuclphysa.2004.10.022
2005SH34 Eur.Phys.J. C 43, 23 (2005) How should we probe a strongly coupled quark-gluon plasma? NUCLEAR REACTIONS 1H(p, X), 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed jets azimuthal correlations.
doi: 10.1140/epjc/s2005-02162-8
2004BR32 Nucl.Phys. A740, 171 (2004) G.E.Brown, C.-H.Lee, M.Rho, E.Shuryak The (q-bar)q bound states and instanton molecules at T ≥ Tc
doi: 10.1016/j.nuclphysa.2004.04.116
2004BR37 J.Phys.(London) G30, S1275 (2004) G.E.Brown, C.-H.Lee, M.Rho, E.Shuryak The instanton molecule liquid and 'sticky molasses' above Tc
doi: 10.1088/0954-3899/30/8/107
2004FA33 Fizika(Zagreb) B 13, 193 (2004) P.Faccioli, A.Schwenk, E.V.Shuryak Instanton contribution to the pion and proton electromagnetic form factors at Q2 ≥ 1 GeV2 NUCLEAR STRUCTURE 1H; calculated electromagnetic form factors, instaton contribution.
2004SH03 Phys.Rev. D 69, 014011 (2004) Understanding nonperturbative deep-inelastic scattering: Instanton-induced inelastic dipole-dipole cross section
doi: 10.1103/PhysRevD.69.014011
2004SH06 Phys.Rep. 391, 381 (2004) Applying the many-body theory to quarks and gluons
doi: 10.1016/j.physrep.2003.10.011
2004SH20 Prog.Part.Nucl.Phys. 53, 273 (2004) Why does the quark-gluon plasma at RHIC behave as a nearly ideal fluid?
doi: 10.1016/j.ppnp.2004.02.025
2004SH30 J.Phys.(London) G30, S1221 (2004) A strongly coupled quark-gluon plasma
doi: 10.1088/0954-3899/30/8/094
2004SH32 Phys.Rev. C 70, 021901 (2004) Rethinking the properties of the quark-gluon plasma at Tc < T < 4Tc
doi: 10.1103/PhysRevC.70.021901
2004SH38 Phys.Rev. D 70, 054507 (2004) Toward a theory of binary bound states in the quark-gluon plasma
doi: 10.1103/PhysRevD.70.054507
2003MR01 Acta Phys.Pol. B34, 4241 (2003) Elliptic flow fluctuations
2003SH05 Nucl.Phys. A715, 289c (2003) How Quantum Mechanics of the Yang-Mills Fields may help us understand the RHIC Puzzles
doi: 10.1016/S0375-9474(02)01438-0
2003SH08 Nucl.Phys. A717, 291 (2003) Toward the semiclassical theory of high energy heavy ion collisions
doi: 10.1016/S0375-9474(03)00639-0
2003SH09 Nucl.Phys. A717, 322 (2003) Matter-induced modification of resonances at RHIC freezeout NUCLEAR REACTIONS 1H(p, X), 197Au(197Au, X), E=high; analyzed resonance production data, matter-induced modification of masses, widths, related features.
doi: 10.1016/S0375-9474(03)00672-9
2002FA03 Phys.Rev. D65, 076002 (2002) Proton Electromagnetic Form Factors in the Instanton Liquid Model NUCLEAR STRUCTURE 1H; calculated electric, magnetic form factors.
doi: 10.1103/PhysRevD.65.076002
2002FA15 Phys.Lett. 549B, 93 (2002) P.Faccioli, A.Schwenk, E.V.Shuryak Instanton Contribution to the Proton and Neutron Electric Form Factors NUCLEAR STRUCTURE 1n, 1H; calculated form factors, instanton contributions.
doi: 10.1016/S0370-2693(02)02886-1
2002RA04 Nucl.Phys. A698, 587c (2002) Regeneration of Anti-Protons in Ultrarelativistic Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), 197Au(197Au, X), E=high; calculated antiproton yields, role of inverse-annihilation reaction. Thermal equilibrium approach.
doi: 10.1016/S0375-9474(01)01434-8
2002SH25 Nucl.Phys. A702, 83c (2002) The QCD Phase Diagram, Equation of State, and Heavy Ion Collisions
doi: 10.1016/S0375-9474(02)00691-7
2002SH31 Phys.Rev. C66, 027902 (2002) Azimuthal asymmetry at large pt seem to be too large for a pure "jet quenching"
doi: 10.1103/PhysRevC.66.027902
2002SH34 Phys.Rev. C66, 034905 (2002) Domain Wall Bubbles in High Energy Heavy Ion Collisions
doi: 10.1103/PhysRevC.66.034905
2002TE02 Nucl.Phys. A698, 479c (2002) D.Teaney, J.Lauret, E.V.Shuryak Hydro + Cascade, Flow, the Equation of State, Predictions and Data
doi: 10.1016/S0375-9474(01)01408-7
2001RA13 Phys.Rev.Lett. 86, 2980 (2001) Resolving the Antibaryon-Production Puzzle in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated antiproton-to-proton production ratio vs fireball temperature. Thermal framework, comparison with data.
doi: 10.1103/PhysRevLett.86.2980
2001SH25 Phys.Rev. C63, 064903 (2001) Long-Range Charge Fluctuations and Search for a Quark-Gluon Plasma Signal
doi: 10.1103/PhysRevC.63.064903
2001SH34 Phys.Lett. 515B, 359 (2001) The Instanton/Sphaleron Mechanism of Prompt Gluon Production in High Energy Heavy Ion Collisions at RHIC
doi: 10.1016/S0370-2693(01)00892-9
2001TE02 Phys.Rev.Lett. 86, 4783 (2001) D.Teaney, J.Lauret, E.V.Shuryak Flow at the SPS and RHIC as a Quark-Gluon Plasma Signature
doi: 10.1103/PhysRevLett.86.4783
2000RA02 Phys.Lett. 473B, 13 (2000) Thermal Dilepton Radiation at Intermediate Masses at the CERN-SpS NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed dilepton spectra; deduced thermal component, no anomalous charm enhancement.
doi: 10.1016/S0370-2693(99)01367-2
2000RH01 Nucl.Phys. A676, 273 (2000) M.Rho, E.Shuryak, A.Wirzba, I.Zahed Generalized Mesons in Dense QCD
doi: 10.1016/S0375-9474(00)00190-1
2000SH07 Phys.Rev. C61, 034905 (2000) High Energy Collisions of Strongly Deformed Nuclei: An old idea with a new twist NUCLEAR REACTIONS Pb(Pb, X), U(U, X), E=high; calculated fragment distributions, energy densities; deduced orientation, deformation effects. Monte Carlo calculation.
doi: 10.1103/PhysRevC.61.034905
1999SH49 Nucl.Phys. A661, 119c (1999) What Have We Learned and Want to Learn from Heavy Ion Collisions at CERN SPS ?
doi: 10.1016/S0375-9474(99)85014-3
1999ST29 Phys.Rev. D60, 114028 (1999) M.Stephanov, K.Rajagopal, E.Shuryak Event-by-Event Fluctuations in Heavy Ion Collisions and the QCD Critical Point
doi: 10.1103/PhysRevD.60.114028
1999TE07 Phys.Rev.Lett. 83, 4951 (1999) Unusual Space-Time Evolution for Heavy-Ion Collisions at High Energies Due to the QCD Phase Transition NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated matter density time evolution, pion pair distributions; deduced phase transition effects.
doi: 10.1103/PhysRevLett.83.4951
1998HU05 Phys.Rev. C57, 1891 (1998) Equation of State, Radial Flow, and Freeze-Out in High Energy Heavy Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=11.6 GeV/nucleon; Pb(Pb, X), E=160 GeV/nucleon; calculated energy density vs time, distance, fragment velocity distributions; deduced freeze-out, radial flow related features. Hydrokinetic model. Comparisons with data.
doi: 10.1103/PhysRevC.57.1891
1998SH11 Phys.Lett. 423B, 9 (1998) Event-by-Event Analysis of Heavy Ion Collisions and Thermodynamical Fluctuations
doi: 10.1016/S0370-2693(98)00127-0
1998SH17 Phys.Lett. 430B, 37 (1998) J/ψ Suppression in Heavy Ion Collisions and the QCD Phase Transition NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed data; deduced possible J/ψ supression mechanism.
doi: 10.1016/S0370-2693(98)00490-0
1998SH25 Nucl.Phys. A638, 207c (1998) Equation of State, Flow, Fluctuations and J/ψ Suppression
doi: 10.1016/S0375-9474(98)00414-X
1998SH32 Nucl.Phys. A642, 14c (1998) QCD Phases at High Density and Instantons
doi: 10.1016/S0375-9474(98)00494-1
1998ST27 Phys.Rev.Lett. 81, 4816 (1998) M.Stephanov, K.Rajagopal, E.Shuryak Signatures of the Tricritical Point in QCD
doi: 10.1103/PhysRevLett.81.4816
1997HU06 Phys.Rev. C56, 453 (1997) Dilepton and/or Photon Production in Heavy Ion Collisions and the QCD Transition NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; 197Au(Pb, X), E=160 GeV/nucleon; analyzed pion rapidity spectra, dilepton, photon production yields. Hydrodynamical model.
doi: 10.1103/PhysRevC.56.453
1997KA33 Phys.Rev. C56, 481 (1997) Flow at Brookhaven AGS Energy (11.6 GeV/nucleon): A barometer for high density effects ( Question ) NUCLEAR REACTIONS 197Au(197Au, X), E=11.6 GeV/nucleon; measured proton, pion transverse momentum distributions; deduced azimuthal asymmetry. Relativistic cascade model.
doi: 10.1103/PhysRevC.56.481
1997SH08 Phys.Rev. C55, 961 (1997) Can Dileptons be Observed in Heavy Ion Collisions at Relativistic Heavy Ion Collider Energies ( Questions ) NUCLEAR REACTIONS 197Au(197Au, X), E not given; calculated dilepton invariant masses for semi-leptonic decays of charmed, b quarks.
doi: 10.1103/PhysRevC.55.961
1997SH45 Acta Phys.Hung.N.S. 5, 395 (1997) The Radial Flow, Equation of State and Freeze-Out Phenomena
1997SO23 Phys.Rev.Lett. 79, 2775 (1997) Ψ'/Ψ Ratio in Nucleus-Nucleus Collisions: A measure for the chiral symmetry restoration temperature ( Question ) NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; U(S, X), E not given; analyzed J/Ψ, Ψ' yields; deduced temperature dependence, chiral symmetry related features.
doi: 10.1103/PhysRevLett.79.2775
1996SH16 Nucl.Phys. A606, 201 (1996) Why is a Nucleon Bound ( Question )
doi: 10.1016/0375-9474(96)00210-2
1996SH17 Phys.Rep. 264, 357 (1996) Structure of the QCD Vacuum and Hadrons
doi: 10.1016/0370-1573(95)00048-8
1995HU14 Phys.Rev.Lett. 75, 4003 (1995) Hydrodynamics Near the QCD Phase Transition: Looking for the longest-lived fireball NUCLEAR REACTIONS 197Au(197Au, X), E=11.6-129 GeV/nucleon; calculated central collisions space-time evolution; deduced QCO phase transition related features.
doi: 10.1103/PhysRevLett.75.4003
1995SC45 Phys.Lett. 356B, 147 (1995) Can Hadrons Survive the Chiral Phase Transition ( Question )
doi: 10.1016/0370-2693(95)00835-9
1995XI03 Nucl.Phys. A590, 589c (1995) Physics of the First 0.3 fm/c at RHIC NUCLEAR REACTIONS 1H(p, X), E=relativistic; 197Au(197Au, X), E=200 GeV/nucleon; measured multiple gluon production associated features, relativistic collisions; deduced production mechanism dominance vs simpler processes.
doi: 10.1016/0375-9474(95)00284-8
1994IL02 Phys.Lett. 325B, 263 (1994) Quark-Induced Correlations between Instantons Drive the Chiral Phase Transition
doi: 10.1016/0370-2693(94)90007-8
1994LI11 Phys.Rev. C49, 2203 (1994) Gluon Multiplication in High Energy Heavy Ion Collisions
doi: 10.1103/PhysRevC.49.2203
1994SH23 Phys.Lett. 333B, 316 (1994) Where Do the Excess Photons and Dileptons in SPS Nuclear Collisions Come From ( Question ) NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; analyzed single photon transverse momentum spectra, dilepton yields; deduced mixed phase expansion features.
doi: 10.1016/0370-2693(94)90148-1
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