NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = G.Q.Li Found 61 matches. 2007LI16 J.Exper.Theo.Phys. 104, 431 (2007) The Influence of Spin on Thermodynamical Quantities
doi: 10.1134/S1063776107030089
1999LI36 Prog.Part.Nucl.Phys. 43, 619 (1999) Electromagnetic Probes of Hadron In-Medium Properties in Relativistic Heavy-Ion Collisions
doi: 10.1016/S0146-6410(99)00101-5
1999LI53 Nucl.Phys. (Supplement) A654, 523c (1999) Kaon Production in Heavy-Ion Collisions and Kaon Condensation in Neutron Stars NUCLEAR REACTIONS Ni(Ni, X), E=high; analyzed kaon production data; deduced in-medium properties. Implications for neutron stars discussed.
doi: 10.1016/S0375-9474(00)88492-4
1999TS01 Phys.Rev. C59, 369 (1999); Erratum Phys.Rev. C61, 029903 (2000) K.Tsushima, A.Sibirtsev, A.W.Thomas, G.Q.Li Resonance Model Study of Kaon Production in Baryon-Baryon Reactions for Heavy-Ion Collisions NUCLEAR REACTIONS 1H(p, K+X), (p, K0X), (n, K+X), (n, K0X), E=high; calculated kaon production σ(E) for several channels. 197Au(197Au, X), Ni(Ni, X), E=high; calculated kaon yields. Resonance model, delta-nucleon interactions considered.
doi: 10.1103/PhysRevC.59.369
1998BR26 Acta Phys.Pol. B29, 2309 (1998) G.E.Brown, G.Q.Li, R.Rapp, M.Rho, J.Wambach Medium Dependence of the Vector-Meson Mass: Dynamical and/or Brown-Rho Scaling ? NUCLEAR REACTIONS 197Au(Pb, X), E=158 GeV/nucleon; calculated dilepton mass spectra; deduced dilepton production mechanism features. Dynamical and Brown-Rho scaling compared.
1998CH37 Nucl.Phys. A641, 357 (1998) Seeing Phi Mesons Through Dileptons NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; calculated dilepton invariant mass spectra; deduced kaon, vector meson, medium effects.
doi: 10.1016/S0375-9474(98)00473-4
1998HA34 Phys.Rev. C58, 365 (1998) M.-A.Halasz, J.V.Steele, G.-Q.Li, G.E.Brown Photon Rates for Heavy-Ion Collisions from Hidden Local Symmetry
doi: 10.1103/PhysRevC.58.365
1998LE14 Phys.Rev. C57, 3488 (1998) C.-H.Lee, T.T.S.Kuo, G.Q.Li, G.E.Brown Nuclear Symmetry Energy
doi: 10.1103/PhysRevC.57.3488
1998LI01 Phys.Rev. C57, 434 (1998) K+ Production in Baryon-Baryon and Heavy-Ion Collisions NUCLEAR REACTIONS 1H(p, X), E=high; 197Au(197Au, X), E=1 GeV/nucleon; analyzed K+ production data; deduced NΔ, ΔΔ interactions role. Boson exchange, relativistic transport models.
doi: 10.1103/PhysRevC.57.434
1998LI10 Nucl.Phys. A630, 563c (1998) Electromagnetic Probes of Dense Matter in Heavy-Ion Collisions NUCLEAR REACTIONS Be, 197Au, W(p, X), W, 197Au(S, X), 197Au(Pb, X), E=high; analyzed dilepton spectra; deduced dilepton production features.
doi: 10.1016/S0375-9474(97)00795-1
1998LI12 Nucl.Phys. A632, 153 (1998) Photon Production in Heavy-Ion Collisions at SPS Energies NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; calculated single photon spectra; deduced photon production mechanisms. Transport model. Comparisons with data.
doi: 10.1016/S0375-9474(97)00808-7
1998LI23 Nucl.Phys. A636, 487 (1998) K+ Versus Λ Flow in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Ni(Ni, X), Ru(Ru, X), 197Au(197Au, X), E ≈ 2 GeV/nucleon; analyzed K+, Λ flow, related features. Relativistic transport model.
doi: 10.1016/S0375-9474(98)00206-1
1998LI25 Phys.Rev.Lett. 81, 1572 (1998) Intermediate-Mass Dilepton Production in Heavy-Ion Collisions at 200A GeV NUCLEAR REACTIONS W(p, X), (S, X), E=200 GeV/nucleon; analyzed dilepton production data; deduced role of secondary processes.
doi: 10.1103/PhysRevLett.81.1572
1998LI29 Nucl.Phys. A638, 491c (1998) Intermediate Mass Dilepton Production in Heavy-Ion Collisions at SPS Energies NUCLEAR REACTIONS W(p, X), (S, X), E=high; analyzed dilepton spectra; deduced secondary processes role.
doi: 10.1016/S0375-9474(98)00338-8
1998LI30 Phys.Rev.Lett. 81, 2177 (1998) Li, Brown, and Lee Reply: Comment on 'Kaon production in heavy-ion collisions and maximum mass of neutron stars '
doi: 10.1103/PhysRevLett.81.2177
1998LI34 Phys.Rev. C58, 1393 (1998) Charge Asymmetry of the Nucleon-Nucleon Interaction
doi: 10.1103/PhysRevC.58.1393
1998LI35 Phys.Rev. C58, 1698 (1998) K-/K+ Ratios in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Ni(Ni, X), Ru(Ru, X), 197Au(197Au, X), E=1-2 GeV/nucleon; analyzed K-/K+ ratios vs centrality, transverse mass, rapidity; deduced in-medium properties. Relativistic transport model.
doi: 10.1103/PhysRevC.58.1698
1998LI47 Phys.Rev. C58, 2914 (1998) Intermediate-Mass Dilepton Spectra and the Role of Secondary Hadronic Processes in Heavy-Ion Collisions NUCLEAR REACTIONS W(S, X), E=high; calculated dilepton spectra, emission rates; deduced secondary hadronic processes contributions. Comparison with data.
doi: 10.1103/PhysRevC.58.2914
1998LI52 Phys.Rev. C58, 3153 (1998) Charge Dependence of the Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(n, n), (n, p), (p, p), E < 300 MeV; calculated phase shifts; deduced charge-independence breaking contribution.
doi: 10.1103/PhysRevC.58.3153
1997CH16 Phys.Lett. 401B, 1 (1997) Phi Meson Production Cross Sections in Pion-Baryon and Baryon-Baryon Interactions NUCLEAR REACTIONS 1H(π-, X), E=high; calculated φ-meson production σ. Boron exchange model.
doi: 10.1016/S0370-2693(97)00374-2
1997CH43 Nucl.Phys. A625, 347 (1997) Phi Meson Production in Heavy-Ion Collisions at SIS Energies NUCLEAR REACTIONS 58Ni(58Ni, X), E=1.93 GeV/nucleon; analyzed p, π-, K+, K-, φ rapidity, transverse mass distributions; deduced medium effects.
doi: 10.1016/S0375-9474(97)00198-X
1997LE28 Phys.Lett. 412B, 235 (1997) C.-H.Lee, T.T.S.Kuo, G.Q.Li, G.E.Brown Momentum Dependence of Single Particle Potential in Dirac Brueckner Approach
doi: 10.1016/S0370-2693(97)01058-7
1997LI35 Nucl.Phys. A625, 372 (1997) Kaons in Dense Matter, Kaon Production in Heavy-Ion Collisions, and Kaon Condensation in Neutron Stars NUCLEAR REACTIONS Ni(Ni, X), E=1-2 GeV/nucleon; analyzed proton, pion, kaon rapidity, transverse mass distributions.
doi: 10.1016/S0375-9474(97)00489-2
1997LI37 Phys.Rev.Lett. 79, 5214 (1997) Kaon Production in Heavy-Ion Collisions and Maximum Mass of Neutron Stars NUCLEAR REACTIONS Ni(Ni, X), E=1, 1.8 GeV/nucleon; analyzed kaon spectra; deduced K- effective mass vs nuclear matter density, implications for neutron star mass.
doi: 10.1103/PhysRevLett.79.5214
1996KO53 J.Phys.(London) G22, 1673 (1996) Medium Effects in High Energy Heavy-Ion Collisions
doi: 10.1088/0954-3899/22/12/002
1996KO54 Nucl.Phys. A610, 342c (1996) C.M.Ko, G.Q.Li, G.E.Brown, H.Sorge Enhancement of Low-Mass Dileptons in SPS Heavy-Ion Collisions: Possible evidence for dropping rho meson mass in medium NUCLEAR REACTIONS 9Be(p, X), E=450 GeV; W, 197Au(p, X), E=200 GeV; analyzed dilepton invariant mass spectra. Relativistic transport model.
doi: 10.1016/S0375-9474(96)00368-5
1996LI10 Phys.Lett. 381B, 17 (1996) Kaon Azimuthal Distributions in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; analyzed nucleon, pion azimuthal distribution at mid-rapidity, relativistic collisions. Relativistic transport model.
doi: 10.1016/0370-2693(96)00582-5
1996LI15 Phys.Rev. C54, 844 (1996) p(t) Dependence of Transverse Flow in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E at 10.8 GeV/c/nucleon; calculated transverse mass distribution for particle in same or opposite side of transverse flow; deduced transverse flow strength related features. Transversely moving thermal, relativistic transport models.
doi: 10.1103/PhysRevC.54.844
1996LI26 Nucl.Phys. A606, 568 (1996) Effects of In-Medium Vector Meson Masses on Low-Mass Dileptons from SPS Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; calculated longitudinal, transverse freeze-out flow velocities, baryon resonance, meson abundance, central baryon density time evolution, proton, pion transverse momentum spectra, rapidity distribution, other aspects. Relativistic transport model.
doi: 10.1016/0375-9474(96)00191-1
1996LI29 Phys.Rev. C54, 1897 (1996) Λ Flow in Heavy-Ion Collisions: The role of final-state Interactions NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; analyzed Λ flow; deduced final state interactions role. Relativistic transport model.
doi: 10.1103/PhysRevC.54.1897
1996LI35 Phys.Rev. C54, R2159 (1996) Antikaon Flow in Heavy-Ion Collisions: Effects of absorption and mean-field potential NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; analyzed nucleon flow, antikaon azimuthal distributions; deduced absorption, mean-field potential effects related features.
doi: 10.1103/PhysRevC.54.R2159
1996LI49 Nucl.Phys. A611, 539 (1996) G.Q.Li, C.M.Ko, G.E.Brown, H.Sorge Dilepton Production in Proton-Nucleus and Nucleus-Nucleus Collisions at SPS Energies NUCLEAR REACTIONS Pb, 197Au(Si, X), E=200 GeV; 197Au, 9Be(p, X), E=450 GeV; analyzed dilepton invariant mass spectra. 197Au(Pb, X), E=160 GeV/nucleon; analyzed normalized total dilepton yield. Relativistic transport model.
doi: 10.1016/S0375-9474(96)00318-1
1995KO08 Nucl.Phys. A583, 591c (1995) Hadrons in Dense Matter NUCLEAR REACTIONS Ni(Ni, X), E=1.85 GeV/nucleon; 197Au(197Au, X), E=1 GeV/nucleon; La(La, X), E=1.35 GeV/nucleon; compiled, reviewed kaon, pion, p-bar production data, analyses. Relativistic transport model, medium effects.
doi: 10.1016/0375-9474(94)00732-3
1995LI03 Nucl.Phys. A582, 731 (1995) Can Dileptons Reveal the In-Medium Properties of Vector Mesons ( Question )
doi: 10.1016/0375-9474(94)00500-M
1995LI11 Phys.Rev.Lett. 74, 235 (1995) Kaon Flow as a Probe of the Kaon Potential in Nuclear Medium NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; calculated kaon average transverse momentum vs center-of-mass rapidity, kaon flow parameter vs t. Relativistic transport model.
doi: 10.1103/PhysRevLett.74.235
1995LI19 Phys.Lett. 349B, 405 (1995) Subthreshold Kaon Production and the Nuclear Equation of State NUCLEAR REACTIONS 197Au(197Au, X), E=0.6-1.2 GeV/nucleon; calculated time evolution of total baryon-baryon collisions number, kaon production probability vs E. Equation of state approach.
doi: 10.1016/0370-2693(95)00301-Z
1995LI28 Phys.Lett. 351B, 37 (1995) Enhancement of Low-m(t) Kaons in Heavy Ion Collisions at AGS Energies NUCLEAR REACTIONS Pb(Si, X), E at 14.6 GeV/c/nucleon; analyzed low-m(T) kaons production data; deduced density isomer role. Relativistic transport model.
doi: 10.1016/0370-2693(95)00389-3
1995LI34 Nucl.Phys. A594, 439 (1995) Kaon Production Cross Sections from Baryon-Baryon Interactions NUCLEAR REACTIONS 1H(p, X), E=high; calculated kaon production σ(E). 197Au(197Au, X), E=1 GeV/nucleon; calculated kaon production probability, σ(θ) vs momentum. One-pion plus one-kaon exchange model.
doi: 10.1016/0375-9474(95)00369-C
1995LI35 Nucl.Phys. A594, 460 (1995) Kaon Flow in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; Ni(Ni, X), E=1.45 GeV/nucleon; calculated kaon, proton, pion flow. Relativistic transport model.
doi: 10.1016/0375-9474(95)00377-D
1995LI42 Phys.Rev.Lett. 75, 4007 (1995) Enhancement of Low-Mass Dileptons in Heavy Ion Collisions NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; analyzed low mass dileptons enhancement. Relativistic transport model.
doi: 10.1103/PhysRevLett.75.4007
1994FA01 Phys.Rev. C49, R608 (1994) X.S.Fang, C.M.Ko, G.Q.Li, Y.M.Zheng Medium Effects on Subthreshold Kaon Production in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; analyzed kaon production σ(θ) vs momentum. Relativistic transport model, kaon degrees of freedom.
doi: 10.1103/PhysRevC.49.R608
1994FA08 Nucl.Phys. A575, 766 (1994) X.S.Fang, C.M.Ko, G.Q.Li, Y.M.Zheng The Relativistic Transport Model Description of Subthreshold Kaon Production in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; calculated kaon production σ, momentum spectra. Relativistic transport model.
doi: 10.1016/0375-9474(94)90165-1
1994LI01 Phys.Rev. C49, 566 (1994) Microscopic Calculation of In-Medium Proton-Proton Cross Sections NUCLEAR REACTIONS 1H(p, p), E=50-350 MeV; calculated in-medium σ(θ), σ. 1H(n, n), E=50-350 MeV; calculated in-medium σ.
doi: 10.1103/PhysRevC.49.566
1994LI02 Phys.Rev. C49, 1139 (1994) G.Q.Li, C.M.Ko, X.S.Fang, Y.M.Zheng Subthreshold Antiproton Production in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 28Si(28Si, p-barX), E=2.1 GeV/nucleon; calculated primordial p-bar production probability, differential momentum distribution. Relativistic transport model.
doi: 10.1103/PhysRevC.49.1139
1994LI04 Nucl.Phys. A568, 745 (1994) Microscopic Description of Nucleon-Nucleus Scattering Based on Realistic Nucleon-Nucleon Interactions NUCLEAR REACTIONS 40Ca, 208Pb(polarized p, p), E=300-500 MeV; calculated σ(θ), polarization observables. 208Pb(n, n), E=155 MeV; calculated σ(θ). 208Pb, 63Cu(p, p), 90Zr(n, n), E=100-600 MeV; calculated σ(E). Microscopic nucleon-nucleus optical potential.
doi: 10.1016/0375-9474(94)90358-1
1994LI28 Phys.Rev. C50, 1725 (1994) Antiproton Production in Ni + Ni Collisions at 1.85 GeV/Nucelon NUCLEAR REACTIONS Ni(Ni, X), E=1.85 GeV/nucleon; calculated p-bar momentum spectra, production. Relativistic Vlasov-Uehling-Uhlenbeck model.
doi: 10.1103/PhysRevC.50.1725
1994LI30 Phys.Rev. C50, R2675 (1994) Effects of N(*)(1440) Resonance on Particle Production in Heavy-Ion Collisions at Subthreshold Energies NUCLEAR REACTIONS 197Au(197Au, X), E ≤ 10 GeV/nucleon; calculated kaon, N(*) production probability vs E, impact parameter. 58Ni(58Ni, X), E ≤ 2.1 GeV/nucleon; calculated p-bar, K-bar, N(*) production probability vs E, impact parameter.
doi: 10.1103/PhysRevC.50.R2675
1994LI36 Phys.Lett. 329B, 149 (1994) Subthreshold Antikaon Production in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 59Ni(58Ni, X), E=1.85 GeV/nucleon; 197Au(197Au, X), E=1 GeV/nucleon; calculated anti-kaon production σ. Relativistic transport model, anti-kaon degree of freedom.
doi: 10.1016/0370-2693(94)90752-8
1994LI39 Phys.Lett. 338B, 118 (1994) Quark Condensate in Nuclear Matter
doi: 10.1016/0370-2693(94)91353-6
1993LI27 Phys.Rev. C48, 1062 (1993); Erratum Phys.Rev. C49, 570 (1994) Self-Consistent Relativistic Calculation of Nucleon Mean Free Path NUCLEAR REACTIONS 40Ca(p, p), E=150-450 MeV; calculated nucleon mean free path vs radial distance. Self-consistent relativistic calculation.
doi: 10.1103/PhysRevC.48.1062
1993LI33 Phys.Rev. C48, 1702 (1993) Microscopic Calculation of In-Medium Nucleon-Nucleon Cross Sections NUCLEAR REACTIONS 1H(n, n), E=50-300 MeV; calculated σ(E), σ(θ). In medium estimates, Dirac-Brueckner approach.
doi: 10.1103/PhysRevC.48.1702
1993LI36 Phys.Rev. C48, 2443 (1993) G.Q.Li, R.Machleidt, R.Fritz, H.Muther, Y.Z.Zhuo Relativistic Microscopic Description of Proton-Nucleus Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=150-450 MeV; calculated σ(θ), analyzing power vs θ. Relativistic, microscopic approach.
doi: 10.1103/PhysRevC.48.2443
1993LI41 J.Phys.(London) G19, 1841 (1993) Microscopic Nucleon-Nucleus Optical Potentials at Intermediate Energies NUCLEAR REACTIONS 40Ca, 90Zr(p, p), E=100-500 MeV; calculated nucleon-nucleus potential; deduced optical potential bulk properties. Realistic interactions, Dirac-Brueckner-Hartree-Fock approach.
doi: 10.1088/0954-3899/19/11/012
1990LI01 Phys.Rev. C41, 169 (1990) Optical Potential and the Fusion Barrier of Two Hot Nuclei NUCLEAR STRUCTURE 120Sn, 208Pb, 90Zr; calculated neutron rms radii vs temperature. 120Sn; calculated charge distribution vs radius. NUCLEAR REACTIONS 120Sn, 40Ca(40Ca, 40Ca), 90Zr(90Zr, 90Zr), 208Pb(208Pb, 208Pb), E not given; calculated potential, Coulomb interaction vs temperature, internucleus distance; deduced fusion barrier temperature shifts. Finite temperature, self-consistent semi-classical calculation.
doi: 10.1103/PhysRevC.41.169
1990LI12 Nucl.Phys. A510, 557 (1990) Finite Temperature Self-Consistent Semiclassical Approach to the Temperature Dependence of Properties of Hot Nuclei NUCLEAR STRUCTURE 208Pb, 120Sn, 90Zr, 40Ca; calculated rms radii change, giant resonance energy vs temperature. 208Pb; calculated nucleon density vs temperature. 120Sn; calculated charge distribution vs temperature. Hot nuclei.
doi: 10.1016/0375-9474(90)90066-U
1990LI20 Phys.Rev. C42, 290 (1990) Self-Consistent Semiclassical Sum Rule Approach and the Properties of Giant Resonances NUCLEAR STRUCTURE 208Pb, 40Ca, 60Ni, 90Zr, 120Sn; calculated rms radii, giant resonances. 208Pb; calculated nucleon densities.
doi: 10.1103/PhysRevC.42.290
1990LI23 Nucl.Phys. A515, 273 (1990) The Thermal Self-Consistent Semiclassical Approach and Microscopic Nucleon-Nucleus Optical Potentials at Finite Temperature NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated nucleon densities, mean free path. Thermal self-consistent, semi-classical calculation. NUCLEAR REACTIONS 40Ca, 208Pb(n, n), E not given; calculated potential parameters vs nucleon-nucleus distance. Nucleon densities from thermal self-consistent, semi-classical calculation.
doi: 10.1016/0375-9474(90)90369-W
1989LI01 Phys.Rev. C39, 276 (1989) Self-Consistent Semiclassical Calculation of the Spin-Orbit Contribution to the Nucleus-Nucleus Optical Potential NUCLEAR REACTIONS 48Ca(48Ca, 48Ca), 60Ni(60Ni, 60Ni), (40Ca, 40Ca), 48Ca(40Ca, 40Ca), 90Zr(16O, 16O), E not given; calculated potential parameter vs internucleus distance. Self-consistent, semi-classical approach.
doi: 10.1103/PhysRevC.39.276
1989LI02 J.Phys.(London) G15, 79 (1989) Semiclassical Approach to Centroid Splitting of Giant Resonances on Deformed Nuclei NUCLEAR STRUCTURE 34S, 36Ar, 150,152Sm, 160Gd, 186W, 232Th, 238U; calculated GDR, GQR energy centroids. Semi-classical approach.
doi: 10.1088/0954-3899/15/1/008
1989LI07 Nucl.Phys. A492, 340 (1989) Self-Consistent Semiclassical Calculation of Nucleus-Nucleus Optical Potentials and Fusion Barriers NUCLEAR STRUCTURE 40Ca, 40Ar, 90,92,94Zr, 120,122,124Sn; calculated rms radii. Self-consistent model. NUCLEAR REACTIONS 40,48Ca, 120Sn(40Ca, 40Ca), E not given; calculated potential vs internuclear separation. 90Zr(40Ca, X), 122Sn(40Ar, X), 120Sn, 90Zr(90Zr, X), 124Sn(92Zr, X), (94Zr, X), E not given; calculated fusion barrier.
doi: 10.1016/0375-9474(89)90091-2
1988LI26 J.Phys.(London) G14, 1387 (1988) Self-Consistent Semiclassical Calculation with Extended Skyrme Forces and the Properties of Giant Resonances NUCLEAR STRUCTURE 48Ca, 90Zr, 130Sn, 208Pb; calculated GDR splitting, rms radii. 40Ca calculated rms radius, nucleon effective mass, charge profile. 208Pb; calculated nucleon effective mass, charge profile. Semi-classical approach.
doi: 10.1088/0305-4616/14/11/010
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