NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = Z.Lin Found 99 matches. 2023LI09 Phys.Rev. C 107, 015804 (2023) Z.Lin, A.W.Steiner, J.Margueron Uncertainty quantification for neutrino opacities in core-collapse supernovae and neutron star mergers
doi: 10.1103/PhysRevC.107.015804
2023ME05 Phys.Rev. C 107, 034909 (2023) Semianalytical calculation of the trajectory of relativistic nuclear collisions in the QCD phase diagram
doi: 10.1103/PhysRevC.107.034909
2022WA10 Phys.Rev. C 105, 034912 (2022) H.-S.Wang, G.-L.Ma, Z.-W.Lin, W.-j.Fu Thermodynamics of partonic matter in relativistic heavy-ion collisions from a multiphase transport model
doi: 10.1103/PhysRevC.105.034912
2022YO08 Phys.Rev. C 106, 024902 (2022) G.-C.Yong, B.-A.Li, Z.-G.Xiao, Z.-W.Lin Probing the high-density nuclear symmetry energy with the Ξ-/Ξ0 ratio in heavy-ion collisions at √ sNN ≈ 3 GeV
doi: 10.1103/PhysRevC.106.024902
2022ZH68 Phys.Rev. C 106, 054910 (2022) Left-right splitting of elliptic flow due to directed flow in heavy ion collisions
doi: 10.1103/PhysRevC.106.054909
2021DE06 Phys.Lett. B 814, 136115 (2021) R.T.deSouza, V.Singh, S.Hudan, Z.Lin, C.J.Horowitz Effect of increasing neutron-excess on the fusion cross-section in 12-15C + 12C at above-barrier energies NUCLEAR REACTIONS 12C(12C, X), (13C, X), (14C, X), (15C, X), E(cm)<20 MeV; analyzed available data; deduced fusion σ using the FSUGOLD and NL3 interactions, TDHF model with a SLy4d interaction; deduced the stronger dependence on neutron-excess attributable to dynamics.
doi: 10.1016/j.physletb.2021.136115
2021ME04 Phys.Rev. C 103, 024907 (2021) Calculating the initial energy density in heavy ion collisions by including the finite nuclear thickness
doi: 10.1103/PhysRevC.103.024907
2021SH23 Phys.Rev. C 103, L061301 (2021) G.Z.Shi, J.J.Liu, Z.Y.Lin, H.F.Zhu, X.X.Xu, L.J.Sun, P.F.Liang, C.J.Lin, J.Lee, C.X.Yuan, S.M.Wang, Z.H.Li, H.S.Xu, Z.G.Hu, Y.Y.Yang, R.F.Chen, J.S.Wang, D.X.Wang, H.Y.Wu, K.Wang, F.F.Duan, Y.H.Lam, P.Ma, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.R.Gao, H.Jian, S.X.Zha, F.C.Dai, R.Fan, Q.Q.Zhao, L.Yang, P.W.Wen, F.Yang, H.M.Jia, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, X.H.Zhou, Y.H.Zhang, M.Wang, M.L.Liu, H.J.Ong, W.Q.Yang β-delayed two-proton decay of 27S at the proton-drip line RADIOACTIVITY 27S(β+2p)[from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility, and implanted into three W1-type double-sided silicon strip detectors (DSSDs)]; measured reaction products, E(p), I(p), pp-coin, p(θ), half-life of 27S decay using Si detectors surrounded by HPGe detectors; deduced branching ratio of β+2p decay, identified as a two-proton transition, dominantly sequential, via the isobaric-analog state (IAS) in 27P to the ground state of 25Al.
doi: 10.1103/PhysRevC.103.L061301
2021SU12 Phys.Rev. C 103, 064909 (2021) Light nuclei production in a multiphase transport model for relativistic heavy ion collisions
doi: 10.1103/PhysRevC.103.064909
2021ZH39 Phys.Rev. C 104, 014908 (2021) C.Zhang, L.Zheng, S.Shi, Z.-W.Lin Using local nuclear scaling of initial condition parameters to improve the system size dependence of transport model descriptions of nuclear collisions NUCLEAR REACTIONS 1H(p, X), E=0.0236-13 TeV; Pb(Pb, X)=7.7-200 GeV/nucleon; 1H(Pb, X), E=5.02 TeV/nucleon; Cu(Cu, X), E=200 GeV/nucleon; Xe(Xe, X), E=5.44 TeV/nucleon; calculated charged particle yields and transverse momentum spectra using a multi-phase transport (AMPT) model. Comparison with available experimental data for various collision systems from p+p to Pb+Pb from Large Hadron Collider (LHC) facilities.
doi: 10.1103/PhysRevC.104.014908
2020HE13 Eur.Phys.J. A 56, 123 (2020) Particle productions and anisotropic flows from the AMPT model for Cu+Au collisions at √ sNN = 200 Gev
doi: 10.1140/epja/s10050-020-00128-6
2020HU08 Phys.Rev. C 101, 061601 (2020) S.Hudan, R.T.deSouza, A.S.Umar, Z.Lin, C.J.Horowitz Enhanced dynamics in fusion of neutron-rich oxygen nuclei at above-barrier energies NUCLEAR REACTIONS 12C(16O, X), (17O, X), (18O, X), (19O, X), E(cm)=7-20 MeV; calculated above-barrier fusion σ(E) using static and dynamical microscopic model. Comparison with experimental data, and with CCFULL, TDHF and FHF calculations.
doi: 10.1103/PhysRevC.101.061601
2020LI43 Phys.Rev. C 102, 045801 (2020) Z.Lin, M.E.Caplan, C.J.Horowitz, C.Lunardini Fast neutrino cooling of nuclear pasta in neutron stars: Molecular dynamics simulations
doi: 10.1103/PhysRevC.102.045801
2020SH16 Phys.Rev. C 102, 014906 (2020) T.Shao, J.Chen, C.M.Ko, Z.-W.Lin Enhanced production of strange baryons in high-energy nuclear collisions from a multiphase transport model
doi: 10.1103/PhysRevC.102.014906
2020ZH09 Phys.Rev. C 101, 034905 (2020) L.Zheng, C.Zhang, S.S.Shi, Z.W.Lin Improvement of heavy flavor production in a multiphase transport model updated with modern nuclear parton distribution functions
doi: 10.1103/PhysRevC.101.034905
2020ZH29 Phys.Rev. C 102, 024904 (2020) X.-L.Zhao, G.-L.Ma, Y.-G.Ma, Z.-W.Lin Validation and improvement of the ZPC parton cascade inside a box
doi: 10.1103/PhysRevC.102.024904
2019LI18 Phys.Rev. C 99, 044911 (2019) Charm quarks are more hydrodynamic than light quarks in final-state elliptic flow
doi: 10.1103/PhysRevC.99.044911
2019NA28 Phys.Rev. C 100, 054903 (2019) K.Nayak, S.Shi, N.Xu, Z.-W.Lin Energy dependence study of directed flow in Au+Au collisions using an improved coalescence in a multiphase transport model
doi: 10.1103/PhysRevC.100.054903
2019XU04 Nucl.Phys. A982, 531c (2019) H.-j.Xu, J.Zhao, X.Wang, H.Li, Z.-W.Lin, C.Shen, F.Wang Re-examining the premise of isobaric collisions and a novel method to measure the chiral magnetic effect
doi: 10.1016/j.nuclphysa.2018.11.031
2019ZH27 Phys.Rev. C 99, 054904 (2019) Li.-Y.Zhang, J.-H.Chen, Z.-W.Lin, Y.-G.Ma, S.Zhang Two-particle angular correlations in heavy ion collisions from a multiphase transport model
doi: 10.1103/PhysRevC.99.054904
2019ZH32 Phys.Rev. C 99, 064906 (2019) C.Zhang, L.Zheng, F.Liu, S.Shi, Z.-W.Lin Update of a multiphase transport model with modern parton distribution functions and nuclear shadowing
doi: 10.1103/PhysRevC.99.064906
2018AL10 Nucl.Phys. A972, 18 (2018) J.L.Albacete, F.Arleo, G.G.Barnafoldi, G.Biro, D.d'Enterria, B.Ducloue, K.J.Eskola, E.G.Ferreiro, M.Gyulassy, S.M.Harangozo, I.Helenius, Z.-B.Kang, P.Kotko, S.A.Kulagin, K.Kutak, J.P.Lansberg, T.Lappi, P.Levai, Z.-W.Lin, G.Ma, Y.-Q.Ma, H.Mantysaari, H.Paukkunen, G.Papp, R.Petti, A.H.Rezaeian, P.Ru, S.Sapeta, B.Schenke, S.Schlichting, H.-S.Shao, P.Tribedy, R.Venugopalan, I.Vitev, R.Vogt, E.Wang, X.-N.Wang, R.Xing, R.Xu, B.-W.Zhang, H.-F.Zhang, W.-N.Zhang Predictions for cold nuclear matter effects in p+Pb collisions at √ SNN = 8.16 TeV
doi: 10.1016/j.nuclphysa.2017.11.015
2018FA08 Phys.Rev. C 98, 025801 (2018) F.J.Fattoyev, E.F.Brown, A.Cumming, A.Deibel, C.J.Horowitz, B.-A.Li, Z.Lin Deep crustal heating by neutrinos from the surface of accreting neutron stars NUCLEAR REACTIONS 1H, Fe(p, π+), Fe(α, π+), E=290-550 MeV/nucleon; calculated multiplicity of pion production as a function of beam energy, total energy per accreted nucleon deposited by neutrinos in the inner crust for a neutron star using the four equations of state, total energy deposited by neutrinos into the inner crust; investigated a new mechanism of deep crustal heating of neutron stars in mass-transferring binaries by neutrinos from decay of charged pions produced at the surface of the neutron stars through p+p, p+Fe and α+Fe collisions.
doi: 10.1103/PhysRevC.98.025801
2018LI48 Phys.Rev. C 98, 034908 (2018) Extension of the Bjorken energy density formula of the initial state for relativistic heavy ion collisions
doi: 10.1103/PhysRevC.98.034908
2018LI60 Phys.Rev. C 98, 054907 (2018) H.Li, H.-j.Xu, J.Zhao, Z.-W.Lin, H.Zhang, X.Wang, C.Shen, F.Wang Multiphase transport model predictions of isobaric collisions with nuclear structure from density functional theory NUCLEAR REACTIONS 96Ru(96Ru, X), 96Zr(96Zr, X), E not given; calculated impact parameter probability distributions, mid rapidity charged hadron multiplicity distributions, eccentricity ratios, charged particle multiplicity per participant pair, invariant mass distributions of opposite and same-sign pion pairs, azimuthal anisotropies of charged hadrons using string melting multiphase transport (AMPT-SM) model with the nuclear densities for 96Ru and 96Zr calculated using density functional theory (DFT). Relevance to experiments at the Relativistic Heavy Ion Collider (RHIC-BNL) in 2018.
doi: 10.1103/PhysRevC.98.054907
2018NA04 Phys.Rev. C 97, 024909 (2018) J.L.Nagle, R.Belmont, K.Hill, J.Orjuela Koop, D.V.Perepelitsa, P.Yin, Z.-W.Lin, D.McGlinchey Minimal conditions for collectivity in e+e- p+p collisions
doi: 10.1103/PhysRevC.97.024909
2018VA03 Phys.Rev. C 97, 031601 (2018) J.Vadas, V.Singh, B.B.Wiggins, J.Huston, S.Hudan, R.T.deSouza, Z.Lin, C.J.Horowitz, A.Chbihi, D.Ackermann, M.Famiano, K.W.Brown Probing the fusion of neutron-rich nuclei with re-accelerated radioactive beams NUCLEAR REACTIONS 28Si(39K, X), (47K, X), E=2-3 MeV/nucleon, [ions of 39K from a source, and 47K from a thermalized radioactive beam charge bred in an ion trap, injected into the ReA3 linac at NSCL-MSU facility]; measured reaction products, particles by ΔE-TOF, fusion σ(E); deduced impact of additional neutrons on fusion. Comparison with Wong parametrization, and with different models including coupled-channel calculations using CCFULL code.
doi: 10.1103/PhysRevC.97.031601
2018XU06 Phys.Rev.Lett. 121, 022301 (2018) H.j.Xu, X.Wang, H.Li, J.Zhao, Z.-W.Lin, C.Shen, F.Wang Importance of Isobar Density Distributions on the Chiral Magnetic Effect Search NUCLEAR REACTIONS 96Ru(96Ru, X), 96Zr(96Zr, X), E not given; calculated proton and neutron density distributions, relative differences between RuRu and ZrZr collisions, impact of the chiral magnetic effect.
doi: 10.1103/physrevlett.121.022301
2018XU07 Chin.Phys.C 42, 084103 (2018) H.-J.Xu, J.Zhao, X.-B.Wang, H.-L.Li, Z.-W.Lin, C.-W.Shen, F.-Q.Wang Varying the chiral magnetic effect relative to flow in a single nucleus-nucleus collision NUCLEAR REACTIONS 197Au(197Au, X), Cu(Cu, X), Ru(Ru, X), Zr(Zr, X), Pb(Pb, X), E∼200 GeV/nucleon; calculated elliptic flow with with MC Glauber and Multi-Phase Transport (ampt) model simulations.
doi: 10.1088/1674-1137/42/8/084103
2018ZH41 Phys.Rev. C 98, 034912 (2018) L.-Y.Zhang, J.-H.Chen, Z.-W.Lin, Y.-G.Ma, S.Zhang Two-particle angular correlations in pp and p-Pb collisions at energies available at the CERN Large Hadron Collider from a multiphase transport model
doi: 10.1103/PhysRevC.98.034912
2017HE13 Phys.Rev. C 96, 014910 (2017) Improved quark coalescence for a multi-phase transport model
doi: 10.1103/PhysRevC.96.014910
2017HO05 Phys.Rev. C 95, 025801 (2017) C.J.Horowitz, O.L.Caballero, Z.Lin, E.O'Connor, A.Schwenk Neutrino-nucleon scattering in supernova matter from the virial expansion
doi: 10.1103/PhysRevC.95.025801
2017LI22 Phys.Rev. C 96, 014901 (2017) H.Li, L.He, Z.-W.Lin, D.Molnar, F.Wang, W.Xie Origin of the mass splitting of azimuthal anisotropies in a multiphase transport model
doi: 10.1103/PhysRevC.96.014901
2017LI41 Phys.Rev. C 96, 055804 (2017) Neutrino scattering in supernovae and the universal spin correlations of a unitary gas
doi: 10.1103/PhysRevC.96.055804
2017SI03 Phys.Lett. B 765, 99 (2017) V.Singh, J.Vadas, T.K.Steinbach, B.B.Wiggins, S.Hudan, R.T.deSouza, Z.Lin, C.J.Horowitz, L.T.Baby, S.A.Kuvin, V.Tripathi, I.Wiedenhover, A.S.Umar Fusion enhancement at near and sub-barrier energies in 19O + 12C NUCLEAR REACTIONS 12C(18O, X), (19O, X), E(cm)<20 MeV; measured reaction products; deduced σ. comparison with a state-of-the-art microscopic model.
doi: 10.1016/j.physletb.2016.12.017
2016JI13 Phys.Rev. C 94, 044910 (2016); Erratum Phys.Rev. C 95, 049904 (2017) Rotating quark-gluon plasma in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.94.044910
2016LI26 Phys.Rev. C 93, 051901 (2016) H.Li, L.He, Z.-W.Lin, D.Molnar, F.Wang, W.Xie Origin of the mass splitting of elliptic anisotropy in a multiphase transport model
doi: 10.1103/PhysRevC.93.051901
2016LI48 Nucl.Phys. A956, 316 (2016) Z.-W.Lin, L.He, T.Edmonds, F.Liu, D.Molnar, F.Wang Elliptic Anisotropy ν2 May Be Dominated by Particle Escape instead of Hydrodynamic Flow
doi: 10.1016/j.nuclphysa.2016.01.017
2016LI54 Ann.Nucl.Energy 96, 181 (2016) Z.Lin, Y.Nie, X.Cai, G.Kang, J.Hu, X.Wang, J.Ren, X.Ruan, J.Chen Benchmarking of 232Th evaluation by a 14.8 MeV neutron leakage spectra experiment with slab samples
doi: 10.1016/j.anucene.2016.05.019
2016MA37 Phys.Rev. C 93, 054911 (2016) Predictions for √ sNN = 5.02 TeV Pb + Pb collisions from a multiphase transport model
doi: 10.1103/PhysRevC.93.054911
2016SC09 Phys.Rev. C 93, 065806 (2016) A.S.Schneider, D.K.Berry, M.E.Caplan, C.J.Horowitz, Z.Lin Effect of topological defects on "nuclear pasta" observables
doi: 10.1103/PhysRevC.93.065806
2015LI27 Phys.Rev. C 92, 014313 (2015) Full weak-charge density distribution of 48Ca from parity-violating electron scattering NUCLEAR REACTIONS 48Ca(e, e), E=2 GeV; calculated ground state electromagnetic charge and weak charge densities of 48Ca versus radius, σ(θ), six Fourier Bessel coefficients, full radial structure of weak charge density, neutron density, parity violating asymmetry parameter. Comparison with experimental data. 1n; deduced size, surface thickness, shell oscillations, and saturation density of the neutron distribution.
doi: 10.1103/PhysRevC.92.014313
2014LI35 Phys.Rev. C 90, 014904 (2014) Evolution of transverse flow and effective temperatures in the parton phase from a multiphase transport model
doi: 10.1103/PhysRevC.90.014904
2012HA08 Phys.Rev. C 85, 034905 (2012) Md.R.Haque, Z.-W.Lin, B.Mohanty Multiplicity, average transverse momentum, and azimuthal anisotropy in U + U collisions at √ sNN = 200 GeV using a multiphase transport model
doi: 10.1103/PhysRevC.85.034905
2012LI46 Phys.Scr. T150, 014022 (2012) α-decay calculations of superheavy nuclei with a folded Woods-Saxon potential RADIOACTIVITY 246,248,250,252,254,256Fm, 252,254,256No, 256Rf, 260,266Sg, 264,266,270Hs, 270Ds, 284Cn, 288Fl, 292Lv(α); calculated T1/2. Comparison with experimental data.
doi: 10.1088/0031-8949/2012/T150/014022
2012XU04 Phys.Rev. C 85, 041901 (2012) J.Xu, L.-W.Chen, C.M.Ko, Z.-W.Lin Effects of hadronic potentials on elliptic flows in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.85.041901
2011CH29 Nucl.Phys. A862-863, 308c (2011) Probing UA(1) Restoration with Domain-Wall Fermions
doi: 10.1016/j.nuclphysa.2011.06.010
2010KO26 Nucl.Phys. A834, 253c (2010) Transport model study of deuteron production in relativistic heavy ion collisions NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV; calculated deuteron elliptic flow, σ(E) using hadronic transport model. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.12.052
2009OH06 Phys.Rev. C 80, 064902 (2009) Deuteron production and elliptic flow in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.80.064902
2007LI13 Phys.Rev. C 75, 034609 (2007) Determination of important nuclear fragmentation processes for human space radiation protection
doi: 10.1103/PhysRevC.75.034609
2007PE30 Phys.Rev. C 76, 044326 (2007) J.C.Pei, F.R.Xu, Z.J.Lin, E.G.Zhao α-decay calculations of heavy and superheavy nuclei using effective mean-field potentials RADIOACTIVITY 166,168,170,172,174,176,178,180,182Pt, 172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194,210Pb, 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230Th, 218,220,222,224,226,228,230,232,234,236U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 254,256,258Rf, 258,260,262Sg, 264,266,270Hs, 270Ds, 286,288Fl, 292Lv, 294Og(α); calculated half-lives, deformation parameters, α-clustering spectroscopic factors, comparisons with experimental half-lives.
doi: 10.1103/PhysRevC.76.044326
2005LI62 Phys.Rev. C 72, 064901 (2005) Z.-W.Lin, C.M.Ko, B.-A.Li, B.Zhang, S.Pal Multiphase transport model for relativistic heavy ion collisions NUCLEAR REACTIONS 1H(p, X), Pb(Pb, X), 197Au(197Au, X), E=high; calculated particles transverse momentum, rapidity distributions, collective flow features. Multiphase transport model.
doi: 10.1103/PhysRevC.72.064901
2004CH11 Phys.Rev. C 69, 031901 (2004) Partonic effects on higher-order anisotropic flows in relativistic heavy-ion collisions NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated anisotropic flow parameters vs transverse momentum, partonic effects. Multiphase transport model.
doi: 10.1103/PhysRevC.69.031901
2004LI01 J.Phys.(London) G30, S263 (2004) Kaon interferometry at RHIC from the AMPT model NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated kaon correlation functions. Multi-phase transport model.
doi: 10.1088/0954-3899/30/1/031
2004PA02 Nucl.Phys. A730, 143 (2004) Multistrange baryon production in relativistic heavy ion collisions NUCLEAR REACTIONS Pb(Pb, X), E(cm)=17 GeV/nucleon; 197Au(197Au, X), E(cm)=130 GeV/nucleon; calculated particle yields, transverse mass spectra, slope parameters, multistrange baryon production features. Multiphase transport model.
doi: 10.1016/j.nuclphysa.2003.10.013
2003LI12 Nucl.Phys. A715, 533c (2003) Charmonium absorption in the meson-exchange model
doi: 10.1016/S0375-9474(02)01509-9
2003LI47 Phys.Rev. C 68, 044901 (2003) Quark coalescence and elliptic flow of charm hadrons
doi: 10.1103/PhysRevC.68.044901
2003LI55 Phys.Rev. C 68, 054904 (2003) Deuteron-nucleus collisions in a multiphase transport model NUCLEAR REACTIONS 197Au(d, X), E(cm)=200 GeV/nucleon; calculated charged particle pseudorapidity distributions, transverse momentum spectra; deduced reaction mechanism features. Multiphase transport model.
doi: 10.1103/PhysRevC.68.054904
2002LI02 Phys.Rev. C65, 015203 (2002) Cross Section for Charmonium Absorption by Nucleons
doi: 10.1103/PhysRevC.65.015203
2002LI11 Nucl.Phys. A698, 375c (2002) Z.-W.Lin, S.Pal, C.M.Ko, B.-A.Li, B.Zhang Multiphase Transport Model for Heavy Ion Collisions at RHIC NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=130 GeV/nucleon; calculated particle rapidity distributions, transverse momentum, yields. Multiphase transport model, comparisons with data.
doi: 10.1016/S0375-9474(01)01383-5
2002LI16 Phys.Rev. C65, 034904 (2002) Partonic Effects on the Elliptic Flow at Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=130, 200 GeV/nucleon; calculated elliptic flow features; deduced sensitivity to partonic scattering cross section.
doi: 10.1103/PhysRevC.65.034904
2002LI56 Phys.Rev.Lett. 89, 152301 (2002) Partonic Effects on Pion Interferometry at the Relativistic Heavy-Ion Collider NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=130 GeV/nucleon; calculated two-pion correlation functions, sensitivity to parton-scattering cross section, related features. Multiphase transport model.
doi: 10.1103/PhysRevLett.89.152301
2002LI59 Phys.Rev.Lett. 89, 202302 (2002) Flavor Ordering of Elliptic Flows at High Transverse Momentum
doi: 10.1103/PhysRevLett.89.202302
2002PA38 Nucl.Phys. A707, 525 (2002) Phi Meson Production in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), 197Au(197Au, X), E=high; calculated φ meson associated rapidity spectra, transverse mass; deduced implications for quark-gluon plasma formation. Multiphase transport model, comparison with data.
doi: 10.1016/S0375-9474(02)00992-2
2002ZH15 Phys.Rev. C65, 054909 (2002) B.Zhang, C.M.Ko, B.-A.Li, Z.-W.Lin, S.Pal J/ψ Production in Relativistic Heavy Ion Collisions from a Multiphase Transport Model NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated J/ψ yields, time dependence, related features.
doi: 10.1103/PhysRevC.65.054909
2001KH19 Phys.Rev. C64, 064606 (2001) M.G.Khayat, P.G.Roos, N.S.Chant, A.P.Dvoredsky, H.Breuer, J.J.Kelly, B.S.Flanders, T.M.Payerle, F.Adimi, T.Gu, J.Huffman, A.Klein, T.Dooling, T.Greco, G.S.Kyle, T.Chang, Z.Lin, M.Wang, R.Meier, S.Ritt, K.Koch, J.Konter, S.Kovalev, S.Mango, B.Van Den Brandt, J.Lawrie Analyzing Power Reduction in Quasifree Pion-Nucleon Knockout Reactions NUCLEAR REACTIONS 7Li(π+, π+'p), E=240 MeV; measured σ(E, θ), Ay(θ); deduced spin dependence in Δ-nucleus potential. Polarized target, DWIA calculations.
doi: 10.1103/PhysRevC.64.064606
2001KO34 Phys.Rev.Lett. 86, 5438 (2001) C.M.Ko, V.Koch, Z.-W.Lin, K.Redlich, M.Stephanov, X.-N.Wang Kinetic Equation with Exact Charge Conservation
doi: 10.1103/PhysRevLett.86.5438
2001LI10 J.Phys.(London) G27, 617 (2001) Effective Hadronic Lagrangian for Charm Mesons
doi: 10.1088/0954-3899/27/3/346
2001LI35 Nucl.Phys. A689, 965 (2001) Charm Meson Scattering Cross Sections by Pion and Rho Meson
doi: 10.1016/S0375-9474(00)00611-4
2001LI36 Phys.Rev. C64, 011902 (2001) Z.-W.Lin, S.Pal, C.M.Ko, B.-A.Li, B.Zhang Charged Particle Rapidity Distributions at Relativistic Energies NUCLEAR REACTIONS Pb(Pb, X), E(cm)=17 GeV/nucleon; 197Au(197Au, X), E(cm)=56, 130 GeV/nucleon; calculated charged particle rapidity distributions, yields. Multiphase transport model, comparisons with data.
doi: 10.1103/PhysRevC.64.011902
2001LI47 Phys.Rev. C64, 041901 (2001) Baryon Number Fluctuation and the Quark-Gluon Plasma
doi: 10.1103/PhysRevC.64.041901
2001PA37 Phys.Rev. C64, 042201 (2001) Strangeness Equilibration in Heavy Ion Collisions NUCLEAR REACTIONS Ni(Ni, X), E=1 GeV/nucleon; calculated kaon and antikaon abundances vs time, equilibrium features. Relativistic transport model.
doi: 10.1103/PhysRevC.64.042201
2000LI03 Phys.Rev. C61, 024904 (2000) Hadronic Scattering of Charmed Mesons
doi: 10.1103/PhysRevC.61.024904
2000LI15 Nucl.Phys. A671, 567 (2000) The Role of Gluons in Dilepton Production from the Quark-Gluon Plasma
doi: 10.1016/S0375-9474(99)00833-7
2000LI31 Phys.Rev. C62, 034903 (2000) Model for J/ψ Absorption in Hadronic Matter
doi: 10.1103/PhysRevC.62.034903
2000PA60 Phys.Rev. C62, 061903 (2000) Antiflow of Kaons in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=6 GeV/nucleon; calculated proton, neutral kaon transverse flow, related features; deduced kaon potential features. Relativistic transport model, comparisons with data.
doi: 10.1103/PhysRevC.62.061903
2000ZH16 Phys.Rev. C61, 067901 (2000) B.Zhang, C.M.Ko, B.-A.Li, Z.Lin Multiphase Transport Model for Relativistic Nuclear Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated fragments rapidity distributions. Multiphase transport model.
doi: 10.1103/PhysRevC.61.067901
2000ZH46 Phys.Rev. C62, 054905 (2000) B.Zhang, C.M.Ko, B.-A.Li, Z.Lin, B.-H.Sa J/ψ Suppression in Ultrarelativistic Nuclear Collisions NUCLEAR REACTIONS S(S, X), 197Au(197Au, X), E=high; calculated parton density distributions, J/ψ suppression related features. Multiphase transport model.
doi: 10.1103/PhysRevC.62.054905
1999BB15 Nucl.Phys. A661, 205c (1999) S.A.Bass, M.Bleicher, W.Cassing, A.Dumitru, H.J.Drescher, K.J.Eskola, M.Gyulassy, D.Kharzeev, Y.V.Kovchegov, Z.Lin, D.Molnar, J.Y.Ollitrault, S.Pratt, B.R.Schlei, H.Sorge, J.Rafelski, R.Rapp, D.H.Rischke, J.B.Schaffner, A.M.Snigirev, D.K.Srivastava, J.Stachel, D.Teaney, R.Thews, S.E.Vance, I.Vitev, R.Vogt, X.N.Wang, B.Zhang, J.Zimanyi Last Call for RHIC Predictions
doi: 10.1016/S0375-9474(99)85024-6
1999LI19 Nucl.Phys. B544, 339 (1999) Energy loss Effects on Heavy Quark Production in Heavy-Ion Collisions at √ s = 5.5 A TeV NUCLEAR REACTIONS Pb(Pb, X), E(cm)=5.5 TeV/nucleon; calculated dileptons rapidity, invariant mass; deduced heavy quark supression due to parton energy loss.
doi: 10.1016/S0550-3213(98)00833-5
1998LI04 Phys.Rev. C57, 899 (1998) Energy Loss Effects on Charm and Bottom Production in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated dilepton spectra; deduced charm, bottom quark energy loss effects, related features.
doi: 10.1103/PhysRevC.57.899
1998LI59 Phys.Lett. 444B, 245 (1998); Erratum Phys.Lett. 476B, 488 (2000) Enhancement of Intermediate Mass Dileptons from Charm Decays at SPS Energies NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated dimuon yields from charm decays; deduced enhancement due to rescattering effects.
doi: 10.1016/S0370-2693(98)01389-6
1996LI21 Chin.Phys.Lett. 13, 165 (1996) Mixed Rescaling Model and Direct Photon Production
doi: 10.1088/0256-307X/13/3/002
1996LI30 Phys.Rev.Lett. 77, 1222 (1996) Nuclear Gluon Shadowing Via Continuum Lepton Pairs in p + A at √ s = 200A GeV NUCLEAR REACTIONS 197Au(p, X), E=200 GeV/nucleon; calculated open charm decay associated dilepton spectra.
doi: 10.1103/PhysRevLett.77.1222
1996LI52 Nucl.Phys. A610, 476c (1996) Nuclear Gluon Shadowing via Dileptons from Open Charm Decay in p + A at √ s = 200 AGeV NUCLEAR REACTIONS 197Au(p, X), E=200 GeV; calculated lepton pair spectrum; deduced gluon shadowing function fit. Open charm decay, two different shadowing scenarios.
doi: 10.1016/S0375-9474(96)00380-6
1996RA05 Phys.Rev. C53, 1005 (1996) B.A.Raue, T.A.Greco, M.G.Khayat, F.Adimi, B.van den Brandt, H.Breuer, T.Chang, N.S.Chant, H.Chen, T.A.Dooling, A.P.Dvoredsky, B.S.Flanders, T.Gu, J.P.Haas, P.Hautle, J.Huffman, J.J.Kelly, A.Klein, K.Koch, J.A.Konter, A.I.Kovalev, G.S.Kyle, J.J.Lawrie, Z.Lin, S.Mango, P.Markowitz, R.Meier, T.Payerle, S.Ritt, P.G.Roos, M.Wang Analyzing Powers for 1H(pol)(π+, π+p) at T(π) = 165 and 240 MeV NUCLEAR REACTIONS 1H(π+, π+p), E=165, 240 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevC.53.1005
1995LI05 Phys.Rev. C51, 2177 (1995); Erratum Phys.Rev. C52, 440 (1995) Open Charm as a Probe of Preequilibrium Dynamics in Nuclear Collisions ( Question ) NUCLEAR REACTIONS 197Au(197Au, X), E=high; analyzed charm, anti-charm pairs rapidity distributions. Three different models.
doi: 10.1103/PhysRevC.51.2177
1995LI36 Nucl.Phys. A590, 495c (1995) Open Charm as a Probe of Pre-Equilibrium Dynamics in Nuclear Collisions ( Question ) NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated charm, anti-charm pairs rapidity density, other aspects.
doi: 10.1016/0375-9474(95)00262-Y
1994AL28 Phys.Rev.Lett. 73, 1336 (1994) T.Alteholz, D.Androic, G.Backenstoss, D.Bosnar, H.Breuer, A.Brkovic, H.Dobbeling, T.Dooling, W.Fong, M.Furic, P.A.M.Gram, N.K.Gregory, J.P.Haas, A.Hoffart, C.H.Q.Ingram, A.Klein, K.Koch, J.Kohler, B.Kotlinski, M.Kroedel, G.Kyle, A.Lehmann, Z.N.Lin, G.Mahl, A.O.Mateos, K.Michaelian, S.Mukhopadhyay, T.Petkovic, R.P.Redwine, D.Rowntree, R.Schumacher, U.Sennhauser, N.Simicevic, F.D.Smit, G.van der Steenhoven, D.R.Tieger, R.Trezeciak, H.Ullrich, M.Wang, M.H.Wang, H.J.Weyer, M.Wildi, K.E.Wilson, and the LADS Collaboration Large-Solid-Angle Study of Pion Absorption on 3He NUCLEAR REACTIONS 3He(π+, X), E=118-239 MeV; measured proton energy spectra following absorption; deduced total absorption σ(E), two-, three-nucleon absorption relative contributions. Large acceptance detector system.
doi: 10.1103/PhysRevLett.73.1336
1994CO23 Appl.Radiat.Isot. 45, 1165 (1994) R.Colle, Z.Lin, J.M.R.Hutchinson, F.J.Schima Delayed Isomeric State in 205Pb abd Its Implications for 4πα Liquid Scintillation Spectrometry of 209Po RADIOACTIVITY 209Po(α); measured α-, β-spectra. 205Pb deduced strong evidence for delayed isomeric state. 4π α liquid scintillation spectrometry, isomeric state implications.
doi: 10.1016/0969-8043(94)90032-9
1994LE18 Nucl.Instrum.Methods Phys.Res. B85, 37 (1994) J.A.Leavitt, L.C.McIntyre, Jr., R.S.Champlin, J.O.Stoner, Jr., Z.Lin, M.D.Ashbaugh, R.P.Cox, J.D.Frank Quantification of Beryllium in Thin Films using Proton Backscattering NUCLEAR REACTIONS 9Be(α, α), E=0.5-3 MeV; 9Be(p, p), E=2.4-2.7 MeV; measured σ(E), θ=170.5°. 9Be(p, α), (p, p), (p, d), E=2.475 MeV; measured particle spectra; deduced self-supporting Be foils areal densities.
doi: 10.1016/0168-583X(94)95781-9
1994LI64 Chin.J.Nucl.Phys. 16, No 4, 291 (1994) The Influence of EMC Effect on Large Transverse Momentum Direct Photon Production NUCLEAR STRUCTURE Fe, 2H; calculated EMC ratio. Statistical model of parton.
1993LI44 Nucl.Instrum.Methods Phys.Res. B79, 498 (1993) Z.Lin, L.C.McIntyre, Jr., J.A.Leavitt, M.D.Ashbaugh, R.P.Cox Determination of Nitrogen using the 14N(α, p)17O Nuclear Reaction NUCLEAR REACTIONS 14N(α, p), E=3.4-4 MeV; measured proton yield, θ=135°; deduced nitrogen content in thin films.
doi: 10.1016/0168-583X(93)95398-O
1993LI55 Chin.J.Nucl.Phys. 15, No 3, 276 (1993) Z.Lin, Y.Gan, D.Fu, H.Wu, C.Wu Neutrinoless Double Bata-Decay of 82Se and the BCS Nuclear Wave Function RADIOACTIVITY 82Se(2β); calculated neutrinoless 2β-decay T1/2; deduced Majorana neutrino mass, right handed current mixing parameter upper limits. Fit to data, BCS wave functions.
1992MC03 Nucl.Instrum.Methods Phys.Res. B64, 457 (1992) L.C.McIntyre, Jr., J.A.Leavitt, M.D.Ashbaugh, Z.Lin, J.O.Stoner, Jr. Cross Sections for 170.5° Backscattering of 4He by the Isotopes of Boron for 4He Energies between 1.0 and 3.3 MeV NUCLEAR REACTIONS 10B, B(α, α), E=1-3.3 MeV; measured σ relative to Rutherford scattering, large angles; deduced resonance structure. Self-supporting targets.
doi: 10.1016/0168-583X(92)95515-S
1992MC05 Nucl.Instrum.Methods Phys.Res. B66, 221 (1992) L.C.McIntyre, Jr., J.A.Leavitt, M.D.Ashbaugh, Z.Lin, J.O.Stone, Jr. Determination of Boron Using the B(α, p)C Nuclear Reaction at Incident Energies Near 3 MeV NUCLEAR REACTIONS 11,10B(α, p), E=1.4-3.3 MeV; measured relative α-yield; deduced thin film boron content.
doi: 10.1016/0168-583X(92)96154-Q
1990LE06 Nucl.Instrum.Methods Phys.Res. B44, 260 (1990) J.A.Leavitt, L.C.McIntyre, Jr., M.D.Ashbaugh, J.G.Oder, Z.Lin, B.Dezfouly-Arjomandy Cross Sections for 170.5° Backscattering of 4He from Oxygen for 4He Energies between 1.8 and 5.0 MeV NUCLEAR REACTIONS 16O(α, α), E=1.8-5 MeV; measured σ(θ) vs E, backscattering. 20Ne deduced resonances, L, Γ.
doi: 10.1016/0168-583X(90)90637-A
1990TA27 J.Phys.(London) G16, 1697 (1990) Z.-Q.Tan, Z.-J.Lin, P.-N.Yan, C.-E.Wu An Integral Formula for Calculating the Glauber Multiple Scattering Amplitude of Composite Particles NUCLEAR REACTIONS 2H(d, d), 1H(p, p), E=high; calculated differential σ. Glauber amplitude expansion.
doi: 10.1088/0954-3899/16/11/018
1989LE09 Nucl.Instrum.Methods Phys.Res. B40/41, 776 (1989) J.A.Leavitt, L.C.McIntyre, Jr., P.Stoss, J.G.Oder, M.D.Ashbaugh, B.Dezfouly-Arjomandy, Z.-M.Yang, Z.Lin Cross Sections for 170.5° Backscattering of 4He from Carbon for 4He Energies between 1.6 and 5.0 MeV NUCLEAR REACTIONS C(α, α), E=1.6-5 MeV; measured σ(θ=175°) vs E.
doi: 10.1016/0168-583X(89)90476-X
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