NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Z.Y.Zhu Found 40 matches. 2019ZH10 Phys.Rev. C 99, 025804 (2019) Z.-Y.Zhu, A.Li, J.-N.Hu, H.Shen Quark mean-field model for nuclear matter with or without bag
doi: 10.1103/PhysRevC.99.025804
2018ZH13 Phys.Rev. C 97, 035805 (2018) Effects of the nucleon radius on neutron stars in a quark mean field model
doi: 10.1103/PhysRevC.97.035805
2016ZH45 Phys.Rev. C 94, 045803 (2016); Erratum Phys.Rev. C 102, 019905 (2020) Z.-Y.Zhu, A.Li, J.-N.Hu, H.Sagawa Δ(1232) effects in density-dependent relativistic Hartree-Fock theory and neutron stars
doi: 10.1103/PhysRevC.94.045803
2010JI15 Eur.Phys.J. A 44, 465 (2010) W.Z.Jiang, Z.Z.Ren, Z.Q.Sheng, Z.Y.Zhu Sensitivity of de-excitation energies of superdeformed secondary minima to the density dependence of symmetry energy with the relativistic mean-field theory NUCLEAR STRUCTURE 191,192,194Hg, 194,196,198,200Au; calculated ground state and superdeformed secondary minima properties, radii, deformation, neutron skin thickness using relativistic mean field model.
doi: 10.1140/epja/i2010-10962-6
2008WA13 Chin.Phys.Lett. 25, 2831 (2008) Phenomenological Study of 3He Photodisintegration up to 150 MeV NUCLEAR REACTIONS 3He(γ, p), E=9-150 MeV; analyzed cross sections.
doi: 10.1088/0256-307X/25/8/027
2005CH09 Chin.Phys.Lett. 22, 302 (2005) B.-Q.Chen, Z.Yu.Ma, Z.-Y.Zhu, H.-Q.Song, Y.-L.Zhao Deformed Potential Energy of Super Heavy Element Z = 120 in a Generalized Liquid Drop Model NUCLEAR REACTIONS 244Pu(58Fe, X), 208Pb(88Sr, X), (94Sr, X), 166Dy(136Xe, X), 252Fm(50Ca, X), E not given; calculated deformed potential energies for fusion reactions. Generalized liquid drop model.
doi: 10.1088/0256-307X/22/2/010
2005JI06 Eur.Phys.J. A 25, 29 (2005) W.Z.Jiang, Z.Z.Ren, T.T.Wang, Y.L.Zhao, Z.Y.Zhu Relativistic mean-field study for Zn isotopes NUCLEAR STRUCTURE 52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75Zn; calculated binding energies, radii, deformation. Relativistic mean-field approach.
doi: 10.1140/epja/i2004-10235-1
2005JI07 Phys.Rev. C 72, 024313 (2005) W.Z.Jiang, Y.L.Zhao, Z.Y.Zhu, S.F.Shen Role of ρNN tensor coupling and 2s1/2 occupation in light exotic nuclei NUCLEAR STRUCTURE 23,24O, 24,25F, 25,26Ne, 138Ba, 208Pb; calculated neutron skin thickness, radii, neutron and proton density distributions, role of tensor coupling and pairing correlations. Relativistic mean field approach.
doi: 10.1103/PhysRevC.72.024313
2004AN06 Chin.Phys.Lett. 21, 895 (2004) Nuclear Fusion Induced by Coulomb-Hydrodynamic Explosion of Deuterium Clusters in Intense Laser Pulses
doi: 10.1088/0256-307X/21/5/037
2004MA07 J.Phys.(London) G30, 13 (2004) Y.G.Ma, D.D.Han, W.Q.Shen, X.Z.Cai, J.G.Chen, Z.J.He, J.L.Long, G.L.Ma, K.Wang, Y.B.Wei, L.P.Yu, H.Y.Zhang, C.Zhong, X.F.Zhou, Z.Y.Zhu Statistical nature of cluster emission in nuclear liquid-vapour phase coexistence NUCLEAR STRUCTURE 129Xe; calculated cluster emission probability from excited nucleus. Isospin-dependent lattice gas model.
doi: 10.1088/0954-3899/30/2/002
2004MA90 Phys.Lett. B 604, 170 (2004) Z.-Y.Ma, J.Rong, B.-Q.Chen, Z.-Y.Zhu, H.-Q.Song Isospin dependence of nucleon effective mass in Dirac Brueckner-Hartree-Fock approach
doi: 10.1016/j.physletb.2004.11.004
2004WA09 Chin.Phys.Lett. 21, 453 (2004) T.-T.Wang, W.-Z.Jiang, W.Zhang, K.Wang, Z.-Y.Zhu Properties of the Alpha Decay Chain Nuclei of 310126, 292120 and 298114 NUCLEAR STRUCTURE 314128, 310126, 306124, 302122, 298120, 294og, 290Lv, 286Fl, 282Cn, 278Ds, 274Hs; calculated binding energies, radii, deformation parameters, Qα. 296122, 292120, 288Og, 284,302Lv, 280,298Fl, 276,294Cn, 272,290Ds, 268,286Hs, 264,282Sg, 260,278Rf, 256,274No, 270Fm, 266Cf; calculated binding energies, Qα. Comparison with previous results.
doi: 10.1088/0256-307X/21/3/010
2004WA20 Chin.Phys.Lett. 21, 1479 (2004) T.-T.Wang, W.-Z.Jiang, Z.-Y.Zhu, Y.-L.Zhao, W.Zhang, J.-G.Chen Occurrence of Superdeformation in Even-Even Isotopes of Zn NUCLEAR STRUCTURE 60,62,64,66,68,70Zn; calculated potential energy surfaces, pairing effects, superdeformation.
doi: 10.1088/0256-307X/21/8/018
2003JI09 Phys.Rev. C 68, 047301 (2003) Particle stability of highly and superdeformed states of Ni, Cu, and Zn isotopes near β stability in relativistic mean-field theory NUCLEAR STRUCTURE 55,57,59,61,63,65,66,67,68,69Ni, 57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73Cu, 59,61,63,65,67,69,71,73Zn; calculated deformation, superdeformed configurations, particle stability features. Relativistic mean-field approach.
doi: 10.1103/PhysRevC.68.047301
2002CA04 Phys.Rev. C65, 024610 (2002) X.Z.Cai, H.Y.Zhang, W.Q.Shen, Z.Z.Ren, J.Feng, D.Q.Fang, Z.Y.Zhu, W.Z.Jiang, Y.G.Ma, C.Zhong, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, Y.T.Zhu, J.C.Wang, J.X.Li, M.Wang, J.F.Wang, Z.J.Ning, Q.J.Wang, Z.Q.Chen Existence of a Proton Halo in 23Al and Its Significance NUCLEAR REACTIONS 12C(19F, X), (20Ne, X), (21Na, X), (22Mg, X), (23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), E ≈ 20-35 MeV/nucleon; measured reaction σ. 23Al deduced proton halo. Comparison with model prediction.
doi: 10.1103/PhysRevC.65.024610
2002CA38 Chin.Phys.Lett. 19, 1068 (2002) X.-Z.Cai, W.-Q.Shen, Z.-Z.Ren, W.-Z.Jiang, D.-Q.Fang, H.-Y.Zhang, C.Zhong, Y.-B.Wei, W.Guo, Y.-G.Ma, Z.-Y.Zhu One-Proton Halo in 31Cl with Relativistic Mean-Field Theory NUCLEAR STRUCTURE 31,32Cl, 30,31S; calculated binding energies, radii, density distributions. 31Cl deduced proton halo. Relativistic mean-field theory.
doi: 10.1088/0256-307X/19/8/312
2002JI01 Phys.Rev. C65, 015210 (2002) W.Z.Jiang, X.J.Qiu, Z.Y.Zhu, Z.J.He Gluonic Contributions in a Four-Fermion Interaction Model
doi: 10.1103/PhysRevC.65.015210
2002ZH30 Nucl.Phys. A707, 303 (2002) H.Y.Zhang, W.Q.Shen, Z.Z.Ren, Y.G.Ma, W.Z.Jiang, Z.Y.Zhu, X.Z.Cai, D.Q.Fang, C.Zhong, L.P.Yu, Y.B.Wei, W.I.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, J.C.Wang, Q.J.Wang, J.X.Li, M.Wang, Z.Q.Chen Measurement of Reaction Cross Section for Proton-Rich Nuclei (A < 30) at Intermediate Energies NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (13N, X), (14N, X), (15N, X), (16N, X), (17N, X), (15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (17F, X), (18F, X), (19F, X), (20F, X), (21F, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (21Na, X), (22Na, X), (23Na, X), (24Na, X), (22Mg, X), (23Mg, X), (24Mg, X), (25Mg, X), (26Mg, X), (23Al, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (27P, X), (28P, X), (29S, X), E=18-33 MeV; measured reaction σ. 17F, 23Al, 27P deduced radii, halo features. Secondary beams from 36Ar fragmentation. Comparison with model predictions.
doi: 10.1016/S0375-9474(02)01007-2
2002ZH49 Prog.Theor.Phys.(Kyoto), Suppl. 146, 33 (2002) H.-Y.Zhang, W.-Q.Shen, Z.-Z.Ren, Y.-G.Ma, X.-Z.Cai, D.-Q.Fang, Z.-Y.Zhu, W.-Z.Jiang, C.Zhong, L.-P.Yu, Y.-B.Wei, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-S.Wang, J.-C.Wang, Q.-J.Wang, J.-X.Li, M.Wang, Z.-Q.Chen Possible Proton Halo and Skin in Light Proton-Rich Nucleus NUCLEAR REACTIONS C(15N, X), (17N, X), (16O, X), (18O, X), (17F, X), (19F, X), (21F, X), (20Ne, X), (22Ne, X), (21Na, X), (23Na, X), (22Mg, X), (24Mg, X), (23Al, X), (25Al, X), (26Si, X), (27P, X), E=30 MeV/nucleon; measured reaction σ. 17F deduced proton skin features. 23Al, 27P deduced proton halo features. Transmission method, Glauber model analysis, relativistic density-dependent Hartree calculations.
doi: 10.1143/PTPS.146.33
2001CA43 Chin.Phys.Lett. 18, 1189 (2001) X.-Z.Cai, W.-Q.Shen, J.Feng, D.-Q.Fang, Z.-Y.Zhu, W.-Z.Jiang, Y.-G.Ma, H.-Y.Zhang, C.Zhong, L.-P.Yu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, J.-S.Wang, Y.-T.Zhu, J.-C.Wang, J.-X.Li, M.Wang, J.-F.Wang, Z.-J.Ning, Q-J.Wang, Z.-Q.Chen Total Reaction Cross Section Measurements at Intermediate Energy for the Proton Halo Candidate 23Al and Its Neighbours NUCLEAR REACTIONS C(19F, X), (20Ne, X), (21Na, X), (22Mg, X), (23Al, X), E ≈ 25-36 MeV/nucleon; measured reaction σ. 23Al deduced possible halo features. Secondary beams from 36Ar fragmentation.
doi: 10.1088/0256-307X/18/9/311
2001FA23 Eur.Phys.J. A 12, 335 (2001) D.Q.Fang, W.Q.Shen, J.Feng, X.Z.Cai, H.Y.Zhang, Y.G.Ma, C.Zhong, Z.Y.Zhu, W.Z.Jiang, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, J.Q.Wang, J.X.Li, M.Wang, J.F.Wang, Z.J.Ning, Q.J.Wang, Z.Q.Chen Evidence for a Proton Halo in 27P Through Measurements of Reaction Cross-Sections at Intermediate Energies NUCLEAR REACTIONS 12C(19O, X), (20F, X), (21F, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Na, X), (24Na, X), (23Mg, X), (25Mg, X), (26Mg, X), (24Al, X), (25Al, X), (26Al, X), (27Al, X), (28Al, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (27P, X), (28P, X), (29S, X), E=30 MeV/nucleon; measured reaction σ following fragmentation of 36Ar primary beam. 27P deduced proton-halo characteristics, neutron, proton and matter radii. Comparison with Glauber model calculations.
doi: 10.1007/s100500170011
2001MB04 Chin.Phys.Lett. 18, 897 (2001) Y.-G.Ma, W.-Q.Shen, Z.-Y.Zhu, H.-Y.Zhang, L.-P.Yu, X.-Z.Cai, D.-Q.Fang, C.Zhong Poissonian Reducibility and Thermal Scaling in Nuclear Dissociation NUCLEAR STRUCTURE 129Xe; calculated fragments isotopic distributions vs temperature for dissociation of excited nucleus. Lattice gas model, Poissonian reducibility.
2001WA38 Nucl.Phys. A691, 618 (2001) J.S.Wang, W.Q.Shen, Z.Y.Zhu, J.Feng, Z.Y.Guo, W.L.Zhan, G.Q.Xiao, X.Z.Cai, D.Q.Fang, H.Y.Zhang, Y.G.Ma RMF Calculation and Phenomenological Formulas for the rms Radii of Light Nuclei NUCLEAR STRUCTURE Z=3-16; A=6-40; calculated radii, binding energies. Relativistic mean field approach, comparisons with data.
doi: 10.1016/S0375-9474(01)00591-7
2000CH19 Phys.Rev. C61, 067601 (2000) L.-W.Chen, F.-S.Zhang, Z.-Y.Zhu Isospin Effects on Rotational Flow in Intermediate Energy Heavy Ion Collisions NUCLEAR REACTIONS 58Fe(58Fe, X), 58Ni(58Ni, X), E=40 MeV/nucleon; calculated in-plane rotational flow features; deduced isospin dependence. Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.61.067601
2000ZH26 Prog.Theor.Phys.(Kyoto), Suppl. 138, 32 (2000) F.-S.Zhang, L.-W.Chen, Z.-Y.Ming, Z.-Y.Zhu A Novel Algorithm to the Transient State of Nuclear Matter with Isospin Asymmetry, Thermal Excitation, and Compression
doi: 10.1143/PTPS.138.32
2000ZH48 Eur.Phys.J. A 9, 149 (2000) F.-S.Zhang, L.-W.Chen, W.-F.Li, Z.-Y.Zhu Isospin Effects on Squeeze-Out Flow in Heavy-Ion Collisions NUCLEAR REACTIONS 124Sn(124Sn, X), 124Ba(124Ba, X), E=150-550 MeV/nucleon; calculated fragments squeeze-out flow angular distributions, related features; deduced isospin dependence. Isospin-dependent quantum molecular dynamics.
doi: 10.1007/s100500070029
1999CH22 Phys.Lett. 459B, 21 (1999) L.-W.Chen, F.-S.Zhang, G.-M.Jin, Z.-Y.Zhu Isospin Dependence of Radial Flow in Heavy-Ion Collisions at Intermediate Energies NUCLEAR REACTIONS 124Sn(124Sn, X), 124Ba(124Ba, X), E=100, 150, 200, 600 MeV/nucleon; calculated fragments mean kinetic energy vs charge, radial flow features; deduced isospin effects. Isospin-dependent QMD.
doi: 10.1016/S0370-2693(99)00628-0
1999JI07 Chin.Phys.Lett. 16, 879 (1999) W.-Z.Jiang, Z.-J.He, Z.-Y.Zhu, J-J.Zhang Dilepton Production in an Expanding Hot Baryon-Rich Quark-Gluon Matter NUCLEAR REACTIONS 197Au(197Au, X), E=0.7-200 GeV/nucleon; calculated initial values and time evolution of temperature and quark chemical potential, dilepton yield.
doi: 10.1088/0256-307X/16/12/008
1999ZH37 Phys.Rev. C60, 064604 (1999) F.-S.Zhang, L.-W.Chen, Z.-Y.Ming, Z.-Y.Zhu Isospin Dependence of Nuclear Multifragmentation in 112Sn + 112Sn and 124Sn + 124Sn Collisions at 40 MeV/nucleon NUCLEAR REACTIONS 112Sn(112Sn, X), 124Sn(124Sn, X), E=40 MeV/nucleon; calculated intermediate mass fragment, light charged particle yields, multiplicities; deduced isospin effect. Isospin-dependent quantum molecular dynamics. Comparisons with data.
doi: 10.1103/PhysRevC.60.064604
1997RE11 Chin.Phys.Lett. 14, 259 (1997) Z.-Z.Ren, Z.-Y.Zhu, Y.-H.Cai, Y.-S.Shen, W.-L.Zhan, G.-O.Xu Ground State Properties of Z = 114 Isotopes in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 298,296,294,292,290,288,286,284,282,280,278,276,274,272,270Fl; calculated binding energies, nucleon, matter radii, βp, βn ground-state deformations, two-neutron separation energies. 298Fl; calculated single-particle energies; deduced spherical shell at N=184. Shell model, relativistic mean-field theory.
1996JI08 Chin.Phys.Lett. 13, 416 (1996) W.-Z.Jiang, Z.-Y.Zhu, X.-J.Qiu Relativistic Density-Dependent Hartree Approach for Nuclear Matter in the Chiral-Symmetry-Breaking Model
doi: 10.1088/0256-307X/13/6/005
1996RE10 Phys.Lett. 380B, 241 (1996) Relativistic Mean-Field Study of Mg Isotopes NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated binding energy, nucleon matter radii, deformation, quadrupole moments.
doi: 10.1016/0370-2693(96)00462-5
1996RE19 Nucl.Phys. A605, 75 (1996) Relativistic Mean-Field Study of Exotic Carbon Nuclei NUCLEAR STRUCTURE 9,10,11,12,13,14,15,16,17,18,19,20,21,22C; calculated levels, J, π, binding energy, nucleon, charge, matter radii, nucleon deformation, isotope shifts, nucleon, matter density distributions in some cases. Relativistic mean-field approach.
doi: 10.1016/0375-9474(96)00186-8
1996RE24 J.Phys.(London) G22, 1793 (1996) Relativistic Mean-Field Study of Even-Even Nuclei Near Z = 108 and N = 162 RADIOACTIVITY Z=108-114; N=162-170; calculated α-decay energies. Z=106; Z=108; Z=110; Z=112; Z=114; calculated binding energy, nucleon radii, β2. Relativistic mean-field theory.
doi: 10.1088/0954-3899/22/12/010
1995MA05 Phys.Rev. C51, 1029 (1995) Collective Motion of Reverse-Reaction System in the Intermediate-Energy Domain Via the Quantum-Molecular-Dynamics Approach NUCLEAR REACTIONS 27Al(40Ar, X), E=36 MeV/nucleon; calculated target-like, mid-central, projectile-like rapidities azimuthal distributions, other aspects. Quantum molecular dynamics approach, collective rotation in collisions.
doi: 10.1103/PhysRevC.51.1029
1995ZH16 Z.Phys. A352, 119 (1995) Description of Isovector Giant Dipole Resonances in Relativistic Vlasov Equation at Small Amplitude Limit NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated isovector GDR centroid energies, nucleon correlated strenmgth distribution. Relativistic Vlasov equation, small amplitude limit.
doi: 10.1007/BF01298896
1994CH32 J.Phys.(London) G20, 891 (1994) Equivalence between Stochastic Quantization of a Two-Dimensional BF-Type Topological Field Theory and Three-Dimensional Topological Quantum Field Theory for a Magnetic Monopole
doi: 10.1088/0954-3899/20/6/004
1994ZH12 Phys.Lett. 328B, 1 (1994) Z.Y.Zhu, W.Q.Shen, Y.H.Cai, Y.G.Ma Study of Halo Nuclei with Phenomenological Relativistic Mean Field Approach NUCLEAR STRUCTURE 11Li, 11Be; calculated rms radii, one-, two-neutron separation energies, density distribution. Halo nuclei, relativistic mean field approach.
doi: 10.1016/0370-2693(94)90418-9
1993FE02 Phys.Lett. 305B, 9 (1993) J.Feng, W.Q.Shen, Y.G.Ma, Z.Y.Zhu The Separation Energy Dependence of the Nuclear Reaction Cross Section NUCLEAR REACTIONS 12C(6He, X), (8He, X), (11Be, X), E not given; 12C(11Li, X), E ≤ 1 GeV/nucleon; 12C(12C, X), E ≤ 2 GeV/nucleon; 27Al(12C, X), E ≤ 400 MeV/nucleon; 64Cu(14N, X), E ≤ 1 GeV/nucleon; 40Ca(16O, X), E ≤ 10 MeV/nucleon; calculated reaction σ(E); deduced neutron separation energy role. Coulomb-modified Glauber model.
doi: 10.1016/0370-2693(93)91097-7
1991ZH05 Phys.Lett. 254B, 325 (1991) Vacuum Polarization in a Relativistic Description of Open Shell Nuclei NUCLEAR STRUCTURE 16O, 56Ni, 90Zr, 208Pb; calculated binding energy per particle, mass distribution, charge rms radii. 20Ne, 168Er; calculated binding energy per particle, n, p quadrupole moments, deformation. Shell model, relativistic description.
doi: 10.1016/0370-2693(91)91163-P
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