NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.X.Li Found 39 matches. 2023WA31 Phys.Rev. C 108, 034306 (2023) X.B.Wang, Y.Chen, G.X.Dong, Y.Su, Z.Li, X.Z.Wu, Z.X.Li Role of pairing correlations in the fission process
doi: 10.1103/PhysRevC.108.034306
2022LI16 Phys.Rev. C 105, 034614 (2022) L.-L.Liu, X.-Z.Wu, Y.-J.Chen, C.-W.Shen, Z.-G.Ge, Z.-X.Li Impact of nuclear dissipation on the fission dynamics within the Langevin approach NUCLEAR REACTIONS 237,238,239,240,241,242,243,244Am, 235,236,237,238,239,240,241,242Pu, 233,234,235,236,237,238,239,240Np, 232,233,234,235,236,237,238,239U(n, F), E=14 MeV; calculated fission fragments mass distributions, total kinetic energy (TKE) distributions, influences of the strength of friction tensor on the fragments distributions. Studied systematic dependence of the averaged TKE on the Coulomb parameter. Three-dimensional Langevin approach. Comparison to the evaluated data from ENDF/B-VIII.0 and results calculated with GEF model.
doi: 10.1103/PhysRevC.105.034614
2022LI65 Chin.Phys.C 46, 124101 (2022) L.-L.Liu, X.-Z.Wu, Y.-J.Chen, C.-W.Shen, Z.-X.Li, Z.-G.Ge, N.-C.Shu Influence of the neck parameter on the fission dynamics within the two-center shell model parametrization NUCLEAR REACTIONS 235U(n, F), E=14 MeV; calculated the total kinetic energy (TKE) distributions.
doi: 10.1088/1674-1137/ac8867
2021CO10 Phys.Rev. C 104, 024603 (2021) M.Colonna, Y.-X.Zhang, Y.-J.Wang, D.Cozma, P.Danielewicz, C.M.Ko, A.Ono, M.B.Tsang, R.Wang, H.Wolter, J.Xu, Z.Zhang, L.-W.Chen, H.-G.Cheng, H.Elfner, Z.-Q.Feng, M.Kim, Y.Kim, S.Jeon, C.-H.Lee, B.-A.Li, Q.-F.Li, Z.-X.Li, S.Mallik, D.Oliinychenko, J.Su, T.Song, A.Sorensen, F.-S.Zhang Comparison of heavy-ion transport simulations: Mean-field dynamics in a box
doi: 10.1103/PhysRevC.104.024603
2021GU26 Phys.Rev. C 104, 044329 (2021) X.Guan, Y.Xin, Y.-J.Chen, X.-Z.Wu, Z.-X.Li Impact of pairing interactions on fission in the deformed mean-field plus standard pairing model NUCLEAR STRUCTURE 220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235Th, 222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237U, 224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239Pu; calculated odd-even mass differences using extended pairing model, and compared with experimental values. 226Th; calculated potential-energy surface contour in (ϵ, α3) plane, neutron and proton pairing correction energies as function of ϵ deformation, inner and outer barrier heights, information entropy. 228,229,230,231,232Th, 232,233,234,236U, 236,237,238Pu; calculated root-mean-square deviations of the theoretical inner and outer heights using BCS pairing, and compared with experimental values. Deformed mean-field plus extended pairing model.
doi: 10.1103/PhysRevC.104.044329
2021LI21 Phys.Rev. C 103, 044601 (2021) L.-L.Liu, Y.-J.Chen, X.-Z.Wu, Z.-X.Li, Z.-G.Ge, K.Pomorski Analysis of nuclear fission properties with the Langevin approach in Fourier shape parametrization NUCLEAR REACTIONS 235U(n, F), E=14 MeV; calculated deformation energy contour for 236U in (q2, q3) plane, total kinetic energy (TKE) as function of the heavy fission fragment, mass distribution of fission fragments, mass-energy correlation of the fission fragments, correlations between the distance of the mass centers of two fragments and the heavy fragment mass at the scission point, correlation between neck parameter and the elongation parameter at the scission point. 233,236,238U, 239Pu(n, F), E=14 MeV; calculated fragment mass distributions, total kinetic energy (TKE) and the probability distributions. Langevin approach for nuclear fission within the Fourier shape parametrization, with the potential energy from macroscopic-microscopic model based on Lublin-Strasbourg drop model and Yukawa-folded potential. Comparison with experimental data, and with evaluated data in ENDF/B-VIII.0.
doi: 10.1103/PhysRevC.103.044601
2019LI16 Phys.Rev. C 99, 044614 (2019) L.-L.Liu, X.-Z.Wu, Y.-J.Chen, C.-W.Shen, Z.-X.Li, Z.-G.Ge Study of fission dynamics with a three-dimensional Langevin approach NUCLEAR REACTIONS 233,238U, 239Pu(n, F), E=14 MeV; 235U(n, F), E=thermal, 14, 25, 35, 45, 55 MeV; calculated fragment mass distributions, total kinetic energy (TKE) of heavy mass fragments, fission time distribution, and elongation and averaged nuclear shape at scission for 235U+n at 14 MeV, potential energy surface for 236U. Three-dimensional Langevin model, with the potential energy surface calculated with the macroscopic-microscopic model based on two-center shell model. Comparison with experimental data, results of GEF code and the evaluated data in ENDF/B-VIII.0 library.
doi: 10.1103/PhysRevC.99.044614
2018ZH12 Phys.Rev. C 97, 034625 (2018) Y.-X.Zhang, Y.-J.Wang, M.Colonna, P.Danielewicz, A.Ono, M.B.Tsang, H.Wolter, J.Xu, L.-W.Chen, D.Cozma, Z.-Q.Feng, S.Das Gupta, N.Ikeno, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, S.Mallik, Y.Nara, T.Ogawa, A.Ohnishi, D.Oliinychenko, M.Papa, H.Petersen, J.Su, T.Song, J.Weil, N.Wang, F.g-S.Zhang, Z.Zhang Comparison of heavy-ion transport simulations: Collision integral in a box
doi: 10.1103/PhysRevC.97.034625
2016XU03 Phys.Rev. C 93, 044609 (2016) J.Xu, L.-W.Chen, M.Y.B.Tsang, H.Wolter, Y.-X.Zhang, J.Aichelin, M.Colonna, D.Cozma, P.Danielewicz, Z.-Q.Feng, A.Le Fevre, T.Gaitanos, C.Hartnack, K.Kim, Y.Kim, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, P.Napolitani, A.Ono, M.Papa, T.Song, J.Su, J.-L.Tian, N.Wang, Y.-J.Wang, J.Weil, W.-J.Xie, F.-S.Zhang, G.-Q.Zhang Understanding transport simulations of heavy-ion collisions at 100A and 400A MeV: Comparison of heavy-ion transport codes under controlled conditions
doi: 10.1103/PhysRevC.93.044609
2015LI40 Chin.Phys.C 39, 114101 (2015) Center-of-mass correction and rotational correction in covariant density functional theory NUCLEAR STRUCTURE A=60-116; calculated total binding, rotational correction, microscopic center-of-mass correction energies, quadrupole deformations in even nuclei. 3DRHB model using the PC-PK1 force, comparison with the available data.
doi: 10.1088/1674-1137/39/11/114101
2015LU02 Phys.Rev. C 91, 027304 (2015) K.Q.Lu, Z.X.Li, Z.P.Li, J.M.Yao, J.Meng Global study of beyond-mean-field correlation energies in covariant energy density functional theory using a collective Hamiltonian method NUCLEAR STRUCTURE Z=8-108, N=8-156; calculated contour map of quadrupole dynamical correlation energies by the CEDF-based 5DCH model, with and without PC-PK1 force, discrepancy of the CEDF binding energies by PC-PK1, discrepancy of theoretical S(2n) and S(2p) for 575 even-even nuclei. Covariant energy density functional (CEDF) by solving a five-dimensional collective Hamiltonian (5DCH). Comparison with AME-12 data.
doi: 10.1103/PhysRevC.91.027304
2014WE11 Phys.Rev. C 90, 054613 (2014) K.Wen, F.Sakata, Z.-X.Li, X.-Z.Wu, Y.-X.Zhang, S.-G.Zhou Energy dependence of the nucleus-nucleus potential and the friction parameter in fusion reactions
doi: 10.1103/PhysRevC.90.054613
2013WE07 Phys.Rev.Lett. 111, 012501 (2013) K.Wen, F.Sakata, Z.-X.Li, X.-Z.Wu, Y.-X.Zhang, S.-G.Zhou Non-Gaussian Fluctuations and Non-Markovian Effects in the Nuclear Fusion Process: Langevin Dynamics Emerging from Quantum Molecular Dynamics Simulations
doi: 10.1103/PhysRevLett.111.012501
2012CH33 Int.J.Mod.Phys. E21, 1250073 (2012) Y.-J.Chen, J.Qian, T.-J.Liu, Z.-X.Li, X.-Z.Wu, N.-C.Shu Energy partition in 235U fission reaction induced by thermal neutron NUCLEAR REACTIONS 235U(n, F), E=thermal; 235U(n, F), E=5.55 MeV; analyzed available data; deduced partition of the total excitation energy between fission fragments. Comparison with available data.
doi: 10.1142/S0218301312500735
2012XI01 Nucl.Phys. A873, 1 (2012) J.Xiang, Z.P.Li, Z.X.Li, J.M.Yao, J.Meng Covariant description of shape evolution and shape coexistence in neutron-rich nuclei at N ≈ 60 NUCLEAR STRUCTURE 88,90,92,94,96,98,100,102,104Kr, 88,90,92,94,96,98,100,102,104,106Sr, 90,92,94,96,98,100,102,104,106,108Zr, 92,94,96,98,100,102,104,106,108,110Mo; calculated charge radii, shape coexistence, deformation using covariant density functional. 98Sr, 100Zr; calculated energies vs deformation, B(E0). 98Sr; calculated levels, J, π vs deformation.
doi: 10.1016/j.nuclphysa.2011.10.002
2011LI33 Chin.Phys.C 35, 629 (2011) M.Liu, Z.-X.Li, N.Wang, F.-S.Zhang Exploring nuclear symmetry energy with isospin dependence in neutron skin thickness of nuclei
doi: 10.1088/1674-1137/35/7/006
2011YA04 Int.J.Mod.Phys. E20, 482 (2011) J.M.Yao, Z.X.Li, J.Xiang, H.Mei, J.Meng Low-lying states in 30Mg: A beyond relativistic mean-field investigation NUCLEAR STRUCTURE 30Mg; calculated quadrupole energy surfaces, probability distributions, energies, B(E2). Gogny force, comparison with experimental data.
doi: 10.1142/S0218301311017880
2011YA11 Phys.Rev. C 84, 024306 (2011) J.M.Yao, J.Meng, P.Ring, Z.X.Li, Z.P.Li, K.Hagino Microscopic description of quantum shape fluctuation in C isotopes NUCLEAR STRUCTURE 10,12,14,16,18,20,22C; calculated levels, J, π, B(E2), potential energy surfaces. Covariant density functional (CDF) theory, angular momentum projection (3DAMP), generator coordinate method (GCM). Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024306
2010LI45 Phys.Rev. C 82, 064306 (2010) M.Liu, N.Wang, Z.-X.Li, F.-S.Zhang Nuclear symmetry energy at subnormal densities from measured nuclear masses NUCLEAR STRUCTURE A=20-250; analyzed nuclear symmetry energy coefficients for more that 2000 previously measured masses using liquid drop formula with the contribution of the Wigner term. Comparison with other methods.
doi: 10.1103/PhysRevC.82.064306
2009JI06 Chin.Phys.Lett. 26, 072502 (2009) Y.-J.Jia, Y.-X.Zhang, Z.-X.Li, X.-H.Lu, F.-H.Liu The influence of Isospin Dependence of In-Medium NN Cross Sections on the Ratio of Emitted Neutrons to Protons in HICs
doi: 10.1088/0256-307X/26/7/072502
2009OU03 Chin.Phys.Lett. 26, 052501 (2009) L.Ou, Z.-X.Li, X.-Z.Wu, W.-L.Sun Disentangling the Effects of Thickness of the Neutron Skin and Symmetry Potential in Nucleon Induced Reactions on Sn Isotopes NUCLEAR REACTIONS 112Sn, 132Sn, 112Cd, 132Ba(n, X), E=100 MeV; 112Sn, 132Sn, 112Cd, 132Ba(p, X), E=100 MeV; calculated σ for target nuclei with normal and enlarged neutron skin. Improved molecular dynamics model.
doi: 10.1088/0256-307X/26/5/052501
2009TI01 Chin.Phys.Lett. 26, 062502 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Possible Mechanisms of Ternary Fission in the 197Au+197Au System at 15 AMeV NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; Calculated ternary fission mass distribution, σ. ImQMD model.
doi: 10.1088/0256-307X/26/6/062502
2009TI12 Eur.Phys.J. A 42, 105 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Dynamic potential barrier in the entrance phase of heavy-ion fusion reactions NUCLEAR REACTIONS 100Mo(86Kr, X), E(cm)=153.9, 163.9, 173.9, 183.9, 203.9, 300.9 MeV; calculated fusion potential barrier and reaction mechanism features using an improved quantum molecular dynamics model.
doi: 10.1140/epja/i2009-10850-2
2009TI13 Chin.Phys.C 33, Supplement 1, 109 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Understanding of the dissipation mechanism in ternary fission for the system 197Au+197Au NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; calculated mass number distributions, impact parameter dependence of production probability of ternary fission and average mass number of fragments. Improved quantum molecular dynamics (ImQMD) model.
doi: 10.1088/1674-1137/33/S1/035
2009WU06 Chin.Phys.C 33, Supplement 1, 30 (2009) X.-Z.Wu, J.-L.Tian, K.Zhao, Y.-X.Zhang, Z.-X.Li Study on the formation of the composite system of 238U+238U NUCLEAR REACTIONS 238U(238U, X), E(cm)=680-1880 MeV; calculated potential and translation kinetic energies, single-particle potentials; deduced conditions for giant composite systems.
doi: 10.1088/1674-1137/33/S1/010
2008LU11 Chin.Phys.Lett. 25, 3932 (2008) X.-H.Lu, Y.-X.Zhang, Z.-X.Li, Z.-X.Zhao Equation of State for Isospin Asymmetric Matter of Nucleons and Deltas
doi: 10.1088/0256-307X/25/11/026
2007OU01 Chin.Phys.Lett. 24, 72 (2007) Mechanism of Proton-Induced Reactions on Targets 16O, 27Al, 56Fe, 112Cd, 184W and 208Pb At Ep = 800 MeV NUCLEAR REACTIONS 16O, 27Al, 56Fe, 112Cd, 184W, 208Pb(p, X), E=800 MeV; calculated spallation neutron spectra, σ(E, θ). Improved molecular dynamics model, statistical decay model, comparison with data.
doi: 10.1088/0256-307X/24/1/020
2007TI04 Chin.Phys.Lett. 24, 905 (2007) Modified Woods-Saxon Potential for Heavy-Ion Fusions Reaction NUCLEAR REACTIONS 92Zr(16O, X), (28Si, X), E(cm) ≈ 30-1000 MeV; 208Pb(16O, X), (48Ca, X), E(cm) ≈ 60-220 MeV; calculated interaction potentials, fusion excitation functions. 208Pb(48Ca, xn), (50Ti, xn), (54Cr, xn), (58Fe, xn), (62Ni, xn), (64Ni, xn), (70Zn, xn), 209Bi(58Fe, xn), (64Ni, xn), (70Zn, xn), E(cm) ≈ 160-280 MeV; compiled, analyzed evaporation σ. Modified Woods-Saxon potential.
doi: 10.1088/0256-307X/24/4/016
2007TI11 Chin.Phys.Lett. 24, 2796 (2007) J.-L.Tian, X.-Z.Wu, L.Ou, Z.-X.Li The Average Lifetime of Giant Composite Systems Formed in Strongly Damped Collisions NUCLEAR REACTIONS 238U(238U, X), E(cm)=680-1880 MeV; 250Cf(232Th, X), E(cm)=680-1880 MeV; calculated lifetimes and orientation angle distributions of the composite systems, and fragment charge distributions using the QMD model.
doi: 10.1088/0256-307X/24/10/023
2006LI13 Chin.Phys.Lett. 23, 804 (2006) M.Liu, N.Wang, Z.-X.Li, X.-Z.Wu Neutron Skin Thickness of Nuclei and Effective Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 18O, 48Ca, 114,116,118,120,122,124,132Sn, 208Pb; calculated radii, neutron skin thickness. 38,40,48,56Ca, 82,90,96,116Zr, 92,100,112,130Sn, 180,208,220,240Pb; calculated neutron and proton density distributions. Skyrme energy density functional, comparisons with data.
doi: 10.1088/0256-307X/23/4/012
2005ZH34 Chin.Phys.Lett. 22, 3048 (2005) H.-Q.Zhang, Z.-H.Liu, F.Yang, C.-J.Lin, M.Ruan, Y.-W.Wu, Z.-X.Li, X.-Z.Wu, K.Zhao, N.Wang Dynamical Effects on Sub-barrier Fusion of 40, 48Ca+90, 96Zr NUCLEAR REACTIONS 96Zr(48Ca, X), E=139.75-176 MeV; 96Zr(48Ca, X), E=133.75-170 MeV; measured fusion σ; 90,96Zr(40Ca, X), E ≈ 120-160 MeV; analyzed fusion σ; deduced dynamical effects. Quantum molecular dynamics model calculation.
doi: 10.1088/0256-307X/22/12/017
2003LI44 Chin.Phys.Lett. 20, 1706 (2003) Limiting Temperatures for Finite Nuclear Systems NUCLEAR STRUCTURE A=20-250; calculated mass dependence of limiting temperatures.
doi: 10.1088/0256-307X/20/10/315
2003MA33 Chin.Phys.Lett. 20, 1238 (2003) G.J.Mao, V.N.Kondratyev, A.Iwamoto, Z.X.Li, X.Z.Wu, W.Greiner, I.N.Mikhailov Neutron Star Composition in Strong Magnetic Fields
doi: 10.1088/0256-307X/20/8/315
2003WA18 Chin.Phys.Lett. 20, 1466 (2003) Development of the Neck in Fusion Reactions 40Ca + 90, 96Zr NUCLEAR REACTIONS 90,96Zr(40Ca, X), E(cm) ≈ 85-115 MeV; calculated fusion σ, neck development and nucleon transfer features. Quantum molecular dynamics approach.
doi: 10.1088/0256-307X/20/9/316
2002LI19 Chin.Phys.Lett. 19, 321 (2002) Isospin Effect on Nuclear Stopping in Intermediate Energy Heavy Ion Collisions NUCLEAR REACTIONS 58Ni(58Ni, X), 120Sn(120Sn, X), E < 400 MeV/nucleon; calculated relative parallel, perpendicular fragment distributions; deduced isospin dependence of nuclear stopping. Comparison of hard and soft equations of state.
doi: 10.1016/S0009-2614(02)00715-7
2001FA05 Nucl.Sci.Eng. 137, 89 (2001) Fragment Distribution Analysis of Proton-Induced Reactions with Intermediate Energy using Quantum Molecular Dynamics Plus Fission Models NUCLEAR REACTIONS Pb(p, X)83Rb/205Bi, E=10-2000 MeV; calculated production σ. Pb(p, X), E=322, 660, 759, 1600 MeV; calculated fragments mass distributions. Quantum molecular dynamics plus fission. Comparisons with data.
doi: 10.13182/NSE01-A2177
2000WA34 Chin.Phys.Lett. 17, 711 (2000) N.Wang, X.-Z.Wu, Z.-X.Li, N.Wang, Y.-Z.Zhuo, X.-Q.Sun Behavior of the Lyapunov Exponent and Phase Transition in Nuclei NUCLEAR STRUCTURE 40,50Ca, 208Pb; calculated Lyapunov exponent vs temperature, phase transition features.
2000WA37 Chin.Phys.Lett. 17, 789 (2000) N.Wang, Z.-X.Li, X.-Z.Wu, N.Wang, X.-Q.Sun One- and Two-Neutron Transfer Reactions in 11Be + 208Pb and Mechanism of Lowering Fusion Barrier NUCLEAR REACTIONS 208Pb(11Be, 10Be), (11Be, 9Be), E=3-9 MeV/nucleon; calculated σ; deduced fusion barrier features. Quantum molecular dynamics.
1979LI18 Chin.J.Nucl.Phys. 1, 73 (1979) Li Zhu-Xia, Zhang Xi-Zhen, Sa Ben-Hao, Shi Yi-Jin The Effects of Core Polarization on the Single Particle State in 208Pb NUCLEAR STRUCTURE 208Pb; calculated levels, B(λ), strength distribution. Core polarization, higher order diagram partial summation.
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