NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = N.Wang Found 124 matches. Showing 1 to 100. [Next]2024YA04 Phys.Rev.Lett. 132, 072502 (2024) H.B.Yang, Z.G.Gan, Y.J.Li, M.L.Liu, S.Y.Xu, C.Liu, M.M.Zhang, Z.Y.Zhang, M.H.Huang, C.X.Yuan, S.Y.Wang, L.Ma, J.G.Wang, X.C.Han, A.Rohilla, S.Q.Zuo, X.Xiao, X.B.Zhang, L.Zhu, Z.F.Yue, Y.L.Tian, Y.S.Wang, C.L.Yang, Z.Zhao, X.Y.Huang, Z.C.Li, L.C.Sun, J.Y.Wang, H.R.Yang, Z.W.Lu, W.Q.Yang, X.H.Zhou, W.X.Huang, N.Wang, S.G.Zhou, Z.Z.Ren, H.S.Xu Discovery of New Isotopes 160Os and 156W: Revealing Enhanced Stability of the N=82 Shell Closure on the Neutron-Deficient Side NUCLEAR REACTIONS 106Cd(58Ni, 4n)160Os, E=335 MeV; measured reaction products; deduced new isotopes, σ. The Spectrometer for Heavy Atoms and Nuclear Structure (SHANS), the Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL), China. RADIOACTIVITY 160Os(α), 156W(β+); measured decay products, Eα, Iα; deduced α-particles energies, Q-values, T1/2, α-decay reduced widths, N=82 shell closure toward the proton drip line. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.132.072502
2024YA07 Phys.Rev. C 109, 034608 (2024) Distinguishing fission-like events from deep-inelastic collisions
doi: 10.1103/PhysRevC.109.034608
2024YE01 Phys.Rev. C 109, L021603 (2024) Odd-even stagger in dissipative fission of excited nuclear systems
doi: 10.1103/PhysRevC.109.L021603
2024ZH04 Phys.Rev. C 109, 014608 (2024) M.M.Zhang, Z.Y.Zhang, Z.G.Gan, N.Wang, H.Yao, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, C.L.Yang, Y.L.Tian, Y.S.Wang, J.Y.Wang, Y.H.Qiang, X.L.Wu, S.Y.Xu, X.Y.Huang, Z.C.Li, Z.Zhao, L.C.Sun, H.Zhou, X.Zhang, G.Xie, L.Zhu, J.H.Zheng, Y.J.Li, F.Guan, Z.W.Lu, W.X.Huang, Y.He, H.S.Xu, Z.Z.Ren, S.G.Zhou Experimental cross section study of 40Ca + 175Lu: Searching for new neutron-deficient Pa isotopes
doi: 10.1103/PhysRevC.109.014608
2023CH42 At.Data Nucl.Data Tables 154, 101587 (2023) Y.Chen, H.Yao, M.Liu, J.Tian, P.Wen, N.Wang Systematic study of fusion barriers with energy dependent barrier radius NUCLEAR STRUCTURE Z<92; analyzed available data; deduced fusion barriers, a modified Siwek-Wilczynski (MSW) fusion σ formula.
doi: 10.1016/j.adt.2023.101587
2023DE31 Eur.Phys.J. A 59, 226 (2023) Unusual behavior in the systematics of α-preformation factors above Z, N = 50 doubly magic shell closures RADIOACTIVITY 104,105,106,107,108,109,110Te, 108,109,110,111,112,113I, 108,109,110,111,112,113Xe, 112,114Cs, 114Ba(α); calculated T1/2, α-preformation factors with the dynamical double-folding potential (DDFP) which incorporates the nuclear me dium effect in α-decay. Comparison with available data.
doi: 10.1140/epja/s10050-023-01138-w
2023LE10 Nucl.Phys. A1038, 122707 (2023) Nuclear mass predictions with multi-hidden-layer feedforward neural network NUCLEAR STRUCTURE A<160; analyzed available data; deduced masses using Keras deep learning framework, the feedforward neural network (FNN) model to improve the predictions of the liquid drop model (LDM).
doi: 10.1016/j.nuclphysa.2023.122707
2023WA19 Phys.Lett. B 843, 138010 (2023) Stringent constraints on nuclear dissipation by second-chance survival probability RADIOACTIVITY 231,232Cf, 229,230Cm, 215,216U(SF); calculated fission barriers, second-chance survival probabilities in the framework of the dynamical Langevin equation coupled to a statistical model of particle emission; deduced a new and sensitive observable the friction strength β. Comparison with available data.
doi: 10.1016/j.physletb.2023.138010
2022LI50 Nucl.Instrum.Methods Phys.Res. B529, 56 (2022) F.-L.Liu, C.-Y.He, H.-R.Wang, N.Bo, D.Wu, T.-L.Ma, W.-S.Yang, J.-H.Wei, Z.-Q.Wang, Y.-N.Liu, M.-Z.Song, Y.-T.Liu, B.Guo, N.-Y.Wang Thick-target yield of 17.6 MeV γ ray from the resonant reaction 7Li(p, γ)8Be at Ep =441keV NUCLEAR REACTIONS 7Li(p, γ), E=441 keV; measured reaction products, Eγ, Iγ; deduced thick-target yields. Comparison with available data. The 2x1.7 MV tandem accelerator at China Institute of Atomic Energy (CIAE).
doi: 10.1016/j.nimb.2022.08.005
2022WU02 Nucl.Phys. A1017, 122357 (2022) D.Wu, B.Guo, C.Y.He, W.P.Lin, Z.An, T.L.Ma, F.L.Liu, W.S.Yang, J.H.Wei, Y.C.Li, Y.P.Shen, Q.W.Fan, X.G.Wu, Y.Zheng, T.X.Li, F.Bai, P.Wang, M.L.Qiu, N.Y.Wang Determination of the 74Ge(p, γ)75As reaction rates in p-process nucleosynthesis with in-beam γ spectroscopy NUCLEAR REACTIONS 74Ge(p, γ), E=2.5-4.3 MeV; measured reaction products, Eγ, Iγ; deduced σ, reaction rates. Comparison with TALYS and EMPIRE nuclear reaction codes calculations. The 3 MV tandem accelerator of the Institute of Nuclear Science and Technology, Sichuan University.
doi: 10.1016/j.nuclphysa.2021.122357
2022YE01 Nucl.Phys. A1024, 122477 (2022) Effects of isospin and shell on probing nuclear dissipation with survival probabilities of heavy systems NUCLEAR STRUCTURE 228,234,240U; calculated the survival probability using the Langevin model. Comparison with available data.
doi: 10.1016/j.nuclphysa.2022.122477
2022YE03 Phys.Rev. C 106, 034603 (2022) Isospin effect on first-chance fission probability NUCLEAR STRUCTURE 220,230,240U, 240Cm; calculated first-chance fission probability as a function of the presaddle dissipation strength at 45 evin model calculations. NUCLEAR REACTIONS 206Pb(32S, X)238Cf, E=193.2 MeV; 206Pb(28Si, X)234Cm, E=172.6 MeV; 204Pb(26Mg, X)230Pu, E=143.9 MeV; 184W(40Ar, X)224U, E=202.6 MeV; 204Pb(30S, X)234Cf, E=174.2 MeV; 204Pb(26Si, X)230Cm, E=151 MeV; calculated first-chance fission probability as a function of the presaddle dissipation strength. Stochastic Langevin model calculations.
doi: 10.1103/PhysRevC.106.034603
2022ZH07 Phys.Rev. C 105, 024328 (2022) H.B.Zhou, Z.Y.Li, Z.G.Gan, Z.Y.Zhang, H.Yao, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, J.L.Tian Modeling the fusion process with a modified Woods-Saxon potential in 40Ar-induced fusion reactions NUCLEAR REACTIONS 176Hf(40Ar, 2np)212Ac, (40Ar, 3np)213Ac, (40Ar, 2nα)209Ra, (40Ar, 3nα)210Ra, E=183, 190 MeV; measured reaction products, Eα, Iα; deduced σ(E), theory evaluation factors. Observed α peaks from decays of 211,212,213,213Ra, 214,215Ac. Comparison to density-constrained time-dependent Hartree-Fock theory calculations. Beam from Sector-Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL). 165Ho(40Ar, 4n), E(cm)=130-160 MeV; 169Tm(40Ar, 4n), E(cm)=130-170 MeV; 174Yb(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 175Lu(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 176Hf(40Ar, 4n), (40Ar, 5n), E(cm)=135-165 MeV; 181Ta(40Ar, 4n), E(cm)=130-160 MeV; analyzed σ(E) from 1984VE09.
doi: 10.1103/PhysRevC.105.024328
2022ZH40 Phys.Rev. C 106, L011602 (2022) K.Zhao, Z.Liu, F.S.Zhang, N.Wang, J.Z.Duan Distinct sequential and massive transfer processes for production of neutron-rich N ≈ 126 nuclei in 238U + 198Pt NUCLEAR REACTIONS 238U(198Pt, X)204Pt/204Os/200Re/198W/195Ta, E=8.0 MeV/nucleon; calculated σ, σ(θ), nucleon exchange rates, average lifetimes of the composite systems, distributions of the average number of neutrons evaporated from primary fragments, kinetic energy distributions of primary fragments. Improved quantum molecular dynamics model (ImQMD). Investigated underlying mechanisms responsible for the enhanced production of new neutron-rich nuclei with neutron numbers around 126. Established the role of sequential transfer and massive transfer of nucleons in producing targetlike and projectile like fragments.
doi: 10.1103/PhysRevC.106.L011602
2022ZH45 Phys.Rev. C 106, 024305 (2022) M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou Fine structure in the α decay of the 8+ isomer in 216, 218U RADIOACTIVITY 216,216m,218,218mU(α)[218U from 182W(40Ar, 4n), E=190 MeV, 184W(40Ca, 2nα), E=206 MeV, 216U from 180W(40Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α1-α2-correlations, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.106.024305
2021GU08 Phys.Rev. C 103, 034613 (2021) Selection of the optimal condition for the production of light neutron-rich isotopes in multinucleon transfer reactions NUCLEAR REACTIONS 130Te(64Ni, X), E(cm)=184.27 MeV; 208Pb(64Ni, X), E(cm)=267.64 MeV; 238U(64Ni, X), E(cm)=307.40 MeV; 197Au(40Ar, X), E(cm)=180.37 MeV; 208Pb(40Ar, X), E(cm)=214.70 MeV; 238U(40Ar, X), E(cm)=226.87 MeV; calculated production cross sections of projectile-like fragments in multi-nucleon transfer (MNT) reactions. Dinuclear system model (DNS) with dynamic deformation. Comparison with experimental production cross sections.
doi: 10.1103/PhysRevC.103.034613
2021LI25 At.Data Nucl.Data Tables 140, 101440 (2021) Compilation of recent nuclear ground state charge radius measurements and tests for models COMPILATION Z=4-88; compiled root-mean-square (rms) charge radii measured by laser spectroscopy; deduced magic numbers, linear relationship between the difference of the mirror nuclear charge radii and the isospin asymmetry, accuracies and predictive powers of the WS* and HFB25 models.
doi: 10.1016/j.adt.2021.101440
2021WA13 Phys.Rev. C 103, 024611 (2021) Fission cross sections of heavy nuclei as a probe of nuclear dissipation NUCLEAR STRUCTURE 226,234,242U, 190,200,210Tl; calculated lowering of fission cross sections caused by friction with respect to its standard statistical-model value as a function of the presaddle dissipation strength, fission barriers as function of angular momentum for 226,234,242U using dynamical Langevin equations. Relevance to fission cross sections for high-isospin and low-spin heavy fissioning systems by light radioactive nuclear beams.
doi: 10.1103/PhysRevC.103.024611
2021YA24 Phys.Rev. C 104, 024605 (2021) Influence of the treatment of initialization and mean-field potential on the neutron to proton yield ratios
doi: 10.1103/PhysRevC.104.024605
2021ZH19 Phys.Lett. B 815, 136101 (2021) K.Zhao, Z.Liu, F.S.Zhang, N.Wang Production of neutron-rich N=126 nuclei in multinucleon transfer reactions: Comparison between 136Xe + 198Pt and 238U + 198Pt reactions NUCLEAR REACTIONS 198Pt(136Xe, X), (238U, X)204Pt/203Ir/202Os, E=8 MeV/nucleon; calculated production σ for primary and residual fragments using improved quantum molecular dynamics (ImQMD) model incorporated with the statistical evaporation model (HIVAP code).
doi: 10.1016/j.physletb.2021.136101
2021ZH22 Phys.Rev.Lett. 126, 152502 (2021) Z.Y.Zhang, H.B.Yang, M.H.Huang, Z.G.Gan, C.X.Yuan, C.Qi, A.N.Andreyev, M.L.Liu, L.Ma, M.M.Zhang, Y.L.Tian, Y.S.Wang, J.G.Wang, C.L.Yang, G.S.Li, Y.H.Qiang, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Z.Z.Ren, S.G.Zhou New α-Emitting Isotope 214U and Abnormal Enhancement of α-Particle Clustering in Lightest Uranium Isotopes RADIOACTIVITY 214,216,218U(α) [from 180,182W(36Ar, 4n), 184W(40Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, T1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.
doi: 10.1103/PhysRevLett.126.152502
2021ZH24 Phys.Rev. C 103, 044314 (2021) H.B.Zhou, Z.G.Gan, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Li, C.X.Yuan, S.Huang, X.J.Sun, H.Y.Peng, L.Ou, X.H.Zhou Lifetime measurement for the isomeric state in 213Th NUCLEAR REACTIONS 176Hf(40Ar, xn)213Th/214Th/215Th, E=183, 190 MeV beam from Sector-Focusing Cyclotron of HIRFL-Lanzhou facility, followed by the separation of evaporation residues (ERs) by the SHANS separator and implanted in three position-sensitive silicon strip detectors (PSSDs); measured position, time, and energy of the ERs, Eα, Iα, Eγ, Iγ, (ER)α-, (ER)γ- and (ER)αγ-correlated events. Enriched target. 213,214,215Th; deduced levels, J, π, isomers, half-lives of the isomers in 213,214,215Th. Comparison with previous experimental results for isomer half-lives. Systematics of 13/2+ isomers in N=123 isotones 207Po, 209Rn, 211Ra and 213Th. RADIOACTIVITY 209,210,211,213Ra, 212,213,215Ac, 211,212,213,214,215,216Th(α)[from 176,177,178,179,180Hf(40Ar, xnyp), E=183, 190 MeV, enriched 176Hf with small abundance of other Hf isotopes]; measured Eα, Iα, αγ-correlations.
doi: 10.1103/PhysRevC.103.044314
2020JI01 Phys.Rev. C 101, 014604 (2020) Probing the production mechanism of neutron-rich nuclei in multinucleon transfer reactions NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; 208Pb(132Sn, X), E(cm)=430, 470, 550 MeV; calculated production cross sections of target-like fragments (TLFs) as function of neutron number for Z=78-86 and N=110-135 fragments, probabilities of proton and neutron stripping and pickup channels as functions of impact parameter, production cross sections of the TLFs, contributions of different decay modes in the de-excitation of the excited TLFs in 132Sn+208Pb at E(cm)=550 MeV: fission of heavy nuclei, light charged particle (LCP) emission, and pure neutron evaporation. Three-dimensional time-dependent Hartree-Fock (TDHF) theory and statistical model GEMINI. Comparisons with the results of the GRAZING model, and with experimental data.
doi: 10.1103/PhysRevC.101.014604
2020LI12 Phys.Rev. C 101, 044313 (2020) C.B.Li, G.L.Zhang, C.X.Yuan, G.X.Zhang, S.P.Hu, W.W.Qu, Y.Zheng, H.Q.Zhang, D.Mengoni, D.Testov, J.J.Valiente-Dobon, H.B.Sun, N.Wang, X.G.Wu, G.S.Li, M.Mazzocco, A.Gozzelino, C.Parascandolo, D.Pierroutsakou, M.La Commara, F.Recchia, A.I.Sison, S.Bakes, I.Zanon, S.Aydin, D.Bazzacco New level scheme and shell model description of 212Rn NUCLEAR REACTIONS 209Bi(6Li, 3n)212Rn, E=28, 30, 34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using GALILEO array at the Tandem-XTU accelerator of Legnaro National Laboratory. 212Rn; deduced levels, J, π, multipolarities, B(E2), B(E3), configurations. Comparison with large-scale shell-model calculations with multiparticle configurations. Systematics of low-, and medium-spin levels in N=126 isotones: 210Po, 212Rn, 214Ra and 216Th. Systematics of 3- to 0+ and 15/2- to 9/2+ excitation energies in N=126 and 127 isotones of Z=82-91. NUCLEAR STRUCTURE 212Rn; calculated levels, J, π, amplitudes of shell-model multiparticle configurations for different levels, B(M1), B(E2), B(E3) using large-scale shell-model calculations with multiparticle configurations. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.044313
2020WU05 Phys.Lett. B 805, 135431 (2020) D.Wu, N.Y.Wang, B.Guo, C.Y.He, Y.Tian, X.Tao, T.L.Ma, F.L.Liu, W.S.Yang, J.H.Wei, Y.P.Shen, S.L.Guo, Q.W.Fan, X.G.Wu, Y.Zheng, T.X.Li, Z.Q.Wang, H.L.Luo, Y.N.Liu, M.L.Qiu New measurement of the 74Ge(p, γ)75As reaction cross sections in the p-process nucleosynthesis NUCLEAR REACTIONS 74Ge(p, γ), E(cm)=1-4.5 MeV; measured reaction products, Eγ, Iγ; deduced σ, reaction rates. Comparison with EMPIRE and TALYS nuclear model codes calculations.
doi: 10.1016/j.physletb.2020.135431
2019GU31 Phys.Rev. C 100, 054616 (2019) S.Q.Guo, X.J.Bao, H.F.Zhang, J.Q.Li, N.Wang Effect of dynamical deformation on the production distribution in multinucleon transfer reactions NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=526, 617, 450 MeV; 198Pt(136Xe, X), E(cm)=643; calculated potential energy surfaces (PES), σ for mass distribution of primary products, cross sections of target-like fragments with Z=78-86 and Z=50-58, production cross sections of the N=126 isotones as a function of the atomic number; deduced influences of dynamical deformation on the PES and the mass distribution of the multi-nucleon transfer (MNT) reactions. Calculations based on the framework of the dinuclear system concept. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.054616
2019WA13 Chin.Phys.C 43, 054101 (2019) H-K.Wang, Z.-H.Li, C.-X.Yuan, Z.-Q.Chen, N.Wang, W.Qin, Y.-Q.He Monopole effects, core excitations, and β decay in the A = 130 hole nuclei near 132Sn NUCLEAR STRUCTURE 130In, 130Sn, 130Cd; calculated energy levels, J, π. RADIOACTIVITY 130In, 130Sn, 130Cd(β-); calculated Gamow-Teller transition probability (B(GT)).
doi: 10.1088/1674-1137/43/5/054101
2018GH06 Nucl.Phys. A979, 237 (2018) Systematic study of proximity potentials for heavy-ion fusion cross sections NUCLEAR REACTIONS 24Mg(34S, x), E(cm)=24-33 MeV;30Si(28Si, x), E(cm)=25-37 MeV;40Ca(40Ca, x), E(cm)=47-66 MeV;48Ti(40Ca, x), E(cm)=53-85 MeV;32S(24Mg, x), E(cm)=26-33 MeV;54Fe(35Cl, x), E(cm)=55-82 MeV;72Ge(16O, x), E(cm)=30-52 MeV;186W(16O, x), E(c)=62-98 MeV;92Zr(28Si, x), E(cm)=63-90 MeV;144Sm(16O, x), E(cm)=56-90 MeV; calculated fusion σ using EBDM (Empirical Barrier Distribution Model) with different proximity potentials and also using coupled channels; compared with data; deduced the best of 14 tested proximity potentials.
doi: 10.1016/j.nuclphysa.2018.09.032
2018JI06 Chin.Phys.C 42, 104105 (2018) Production mechanism of neutron-rich nuclei around N=126 in the multi-nucleon transfer reaction 132Sn + 208Pb NUCLEAR REACTIONS 208Pb(132Sn, X), E(cm)=470, 550, 800 MeV; analyzed available data; calculated probabilities for different transfer channels, σ of the target-like fragments using the particle-number projection method, time-dependent Hartree-Fock approach in three dimensions.
doi: 10.1088/1674-1137/42/10/104105
2018LI22 Phys.Rev. C 97, 044606 (2018) L.Li, Y.Zhang, Z.Li, N.Wang, Y.Cui, J.Winkelbauer Impact parameter smearing effects on isospin sensitive observables in heavy ion collisions NUCLEAR REACTIONS 112Sn(112Sn, X), E=35, 50, 70, 120 MeV/nucleon; calculated multiplicity and charge distributions, average impact parameter as function of mass, and averaged real impact parameter. 112Sn(112Sn, X), 124Sn(124Sn, X), 132Sn(124Sn, X), E<80 MeV/nucleon; calculated coalescence invariant single neutron to proton yield ratio, and coalescence invariant double neutron to proton yield ratio; deduced effect of impact parameter smearing on coalescence invariant double neutron to proton yield ratios using SkM* and SLy4 parameter sets. Improved quantum molecular dynamics (ImQMD) model. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.044606
2018LI51 Chin.Phys.C 42, 114101 (2018) Statistical errors in Weizsacker-Skyrme mass model NUCLEAR STRUCTURE 132Sn, 208Pb, Ca, Zr, Sb, Rn; calculated atomic masses; deduced statistical uncertainties of 13 model parameters. Comparison with AME2016.
doi: 10.1088/1674-1137/41/11/114101
2018SU24 Chin.Phys.C 42, 124105 (2018) X.-J.Sun, C.-X.Chen, N.Wang, H.-B.Zhou Systematic description of nuclear electric quadrupole moments NUCLEAR STRUCTURE A=2-260; calculated nuclear electric quadrupole moments. Comparison with available data.
doi: 10.1088/1674-1137/42/12/124105
2018WA02 Phys.Rev. C 97, 014603 (2018) Probing nuclear dissipation with first-chance fission probability NUCLEAR REACTIONS 235U(3He, F)238Pu*, E=41.9 MeV; 235U(α, F)239Pu*, E=66.4 MeV; 239Pu(3He, F)242Cm*, E=42.8 MeV; 239Pu(α, F)243Cm*, E=67.3 MeV; 241Am(3He, F)244Bk*, E=43.1 MeV; 241Am(α, F)245Bk*, E=67.6 MeV; 248Cm(3He, F)251Cf*, E=42.9 MeV; 248Cm(α, F)252Cf*, E=67.3 MeV; calculated average angular momentum contributing to fission using fusion spin distribution formula and the scaling formulas for critical angular momentum and diffuseness for fusion. 220Th, 240Cf; calculated influence of dissipation on first-chance fission probability as a function of the presaddle friction strength at excitation energies of 50 MeV and 80 MeV for 220Th and 240Cf. Stochastic Langevin model.
doi: 10.1103/PhysRevC.97.014603
2018WA27 Phys.Rev. C 98, 034614 (2018) Probing postsaddle dissipation with light-particle multiplicity of hot heavy nuclear systems NUCLEAR STRUCTURE 240Am; calculated proton, neutron, and α-particle multiplicity as a function of postsaddle dissipation strength and angular momenta, for fission of compound nucleus 240Am at an angular momentum of 40 units and at excitation energies of E*=60, 120, and 250 MeV, and fission barrier strength. Dynamical Langevin equations coupled to a statistical decay model.
doi: 10.1103/PhysRevC.98.034614
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
2017LI42 Chin.Phys.C 41, 114101 (2017) Statistical errors in Weizsacker-Skyrme mass model NUCLEAR STRUCTURE 132Sn, 208Pb, Ca, Zr, Sb, Rn; calculated masses. Comparison with AME2003 and AME2016 evaluations.
doi: 10.1088/1674-1137/41/11/114101
2017TI02 Phys.Rev. C 95, 041601 (2017) Constraining presaddle dissipation with fission cross sections of light nuclear systems NUCLEAR STRUCTURE 205Bi, 215Fr, 225Pa, 230Np; calculated drop of fission cross sections over the statistical model values at different angular momenta and excitation energies using stochastic Langevin model.
doi: 10.1103/PhysRevC.95.041601
2017YA02 Phys.Rev. C 95, 014607 (2017) Microscopic dynamics simulations of multinucleon transfer in 86Kr + 64Ni at 25 MeV/nucleon NUCLEAR REACTIONS 64Ni(86Kr, X), E=25 MeV/nucleon; calculated cross sections (or isotopic yield distributions), and differential σ(θ) for Z=30-35 fragments, probability of fusion, binary scattering, and other cases as a function of impact parameter, probability of binary scattering events as a function of impact parameter, distribution of TKEL of fragments, and mass-TKE distribution. Improved quantum molecular dynamics (ImQMD) model, with a statistical code (GEMINI) for describing the secondary decay of fragments. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.014607
2017ZA04 Phys.Rev. C 95, 034620 (2017) Dynamical explanation for the anomaly in the diffuseness parameter of the nucleus-nucleus potential in heavy-ion fusion reactions NUCLEAR REACTIONS 46Ti(40Ca, X), E(cm)=65, 75 MeV; calculated time evolution of density distribution. 92Zr(16O, X), E(cm)=45, 50, 55, 60 MeV; 92Zr(28Si, X), E(cm)=70, 75, 80, 85 MeV; calculated dynamical nucleus-nucleus potentials. 92Zr(12C, X), E(cm)=28-43 MeV; 92Zr(16O, X), E(cm)=37-65 MeV; 92Zr(28Si, X), E(cm)=65-90 MeV; 92Zr(35Cl, X), E(cm)=77-105 MeV; 46Ti(40Ca, X), E(cm)=54-80 MeV; 154Sm(16O, X), E(cm)=52-75 MeV; calculated fusion σ(E), diffuseness parameter as a function of incident energy. Improved quantum molecular dynamics (ImQMD) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.034620
2016JI16 Phys.Rev. C 94, 064301 (2016) H.Jiang, Y.Y.Cheng, N.Wang, Li.-W.Chen, Y.M.Zhao, A.Arima Robustness of the I4 symmetry energy coefficient ATOMIC MASSES A=16-300, Z>8, N>8; analyzed I4 symmetry energy coefficient extracted from popular mass models and corresponding databases improved by the radial basis function (RBF) approach and the RBF with odd-even correction; deduced robust linear correlation between present I4 symmetry energy coefficients and the corresponding rms deviations from experimental masses of these theoretical databases.
doi: 10.1103/PhysRevC.94.064301
2016LI05 Phys.Rev. C 93, 014618 (2016) C.Li, F.Zhang, J.Li, L.Zhu, J.Tian, N.Wang, F.-S.Zhang Multinucleon transfer in the 136Xe + 208Pb reaction NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; calculated density distribution contours as function of time, lifetime of the neck, total-kinetic-energy-mass distributions for different impact parameters, TKEL distributions of primary binary fragments, average excitation energy of projectile-like fragments (PLFs) and target-like fragments (TLFs) as a function of neck lifetime, mass distributions of primary binary fragments at different impact parameters, production cross sections for N=110-140, Pt, Au, Hg, Tl, Pb, Bi, Po and At isotopes. Improved quantum molecular dynamics model (ImQMD) for multinucleon transfer reaction using statistical decay code GEMINI. Comparison with prediction of the dinuclear system and GRAZING model, and with available experimental data.
doi: 10.1103/PhysRevC.93.014618
2016TI06 Chin.Phys.C 40, 094101 (2016) J.-L.Tian, H.-T.Cui, T.Gao, N.Wang Effect of Wigner energy on the symmetry energy coefficient in nuclei NUCLEAR STRUCTURE A=80; calculated nuclear symmetry energy coefficients.
doi: 10.1088/1674-1137/40/9/094101
2016WA02 Phys.Rev. C 93, 014302 (2016) Correlations between neutrons and protons near the Fermi surface and Qαof superheavy nuclei NUCLEAR STRUCTURE Z=14, N=10-40; Z=28, N=20-70; calculated S(n), S(2n) and compared to experimental values. 46Si, 60Ca, 78Ni, 132Sn, 208Pb, 252Fm, 270Hs, 296Og, 298120, 308124; N=30-130 along the shell stability line; calculated scaled shell gaps, shell correction energies and quadrupole deformation β2. 284,285,286,287,288,289Fl, 288,289,290,291,292,293Lv, 292,293,294,295,296,297Og, 296,297,298,299,300,301120, 300,301,302,303,304,305122, 304,305,306,307,308,309124, 308,309,310,311,312,313126; calculated shell correction energies, deformation energies, Q(α). Weizsacker-Skyrme (WS4)mass model. Comparison with other theoretical calculations, and with available experimental values.
doi: 10.1103/PhysRevC.93.014302
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
2016ZH30 Phys.Rev. C 94, 024601 (2016) K.Zhao, Zh.Li, Y.Zhang, N.Wang, Q.Li, C.Shen, Y.Wang, X.Wu Production of unknown neutron-rich isotopes in 238U + 238U collisions at near-barrier energy NUCLEAR REACTIONS 238U(238U, X), E=7.0 MeV/nucleon; calculated production cross sections for primary and residual fragments with charge number from Z=70 to 120, N=100-200 neutron-rich nuclides, average excitation energies of primary fragments of unknown isotopes of uranium; predicted about 60 unknown neutron-rich nuclides from Z=88 to 105 with production cross sections above the lower bound of 10-8 mb. Improved quantum molecular dynamics (ImQMD) model with the statistical evaporation model using HIVAP code.
doi: 10.1103/PhysRevC.94.024601
2015JI06 Phys.Rev. C 91, 054302 (2015) H.Jiang, N.Wang, L.-W.Chen, Y.M.Zhao, A.Arima Model dependence of the I4 term in the symmetry energy for finite nuclei
doi: 10.1103/PhysRevC.91.054302
2015MA27 Phys.Rev. C 91, 044604 (2015) Dynamical and statistical description of multifragmentation in heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=80 MeV; 46Ti(16O, X), E(cm)=38 MeV; 92Zr(16O, X), E(cm)=50 MeV; calculated excitation energy and density distributions of fragments. 197Au(197Au, X), E=35 MeV/nucleon; calculated excitation energies per nucleon, and charge distributions of fragments. Hybrid model of improved quantum molecular dynamics (ImQMD) model plus the statistical model GEMINI. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.044604
2015OU02 Phys.Rev.Lett. 115, 212501 (2015) L.Ou, Z.Xiao, H.Yi, N.Wang, M.liu, J.Tian Dynamic Isovector Reorientation of Deuteron as a Probe to Nuclear Symmetry Energy NUCLEAR REACTIONS 124Sn(polarized d, X), E=100 MeV/nucleon; calculated breakup reaction σ(θ). Comparison with available data.
doi: 10.1103/PhysRevLett.115.212501
2015SU02 Chin.Phys.C 39, 014102 (2015) X.-J.Sun, C.-G.Yu, N.Wang, Y.-X.Yang, C.H.Pan Pre-neutron-emission mass distributions for reaction 238U(n, f) up to 60 MeV NUCLEAR REACTIONS 238U(n, F), E<60 MeV; analyzed available data; deduced σ, preneutron-emission mass distributions, fission yields. Empirical fission potential model, comparison with available data.
doi: 10.1088/1674-1137/39/1/014102
2015TI01 Chin.Phys.C 39, 034102 (2015) Langevin analysis of fission excitation functions induced by protons NUCLEAR REACTIONS 206Pb, 209Bi(p, F), E<200 MeV; analyzed available data; deduced fits to measured excitation function data of fission σ.
doi: 10.1088/1674-1137/39/3/034102
2015WA14 Phys.Rev. C 91, 044308 (2015) N.Wang, M.Liu, H.Jiang, J.L.Tian, Y.M.Zhao Mass dependence of symmetry energy coefficients in the Skyrme force ATOMIC MASSES A=160; A=20-300; A=20-106; analyzed properties of nuclear symmetry energy as function of mass using the extended Thomas-Fermi (ETF2) approximation and 36 different Skyrme forces. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.91.044308
2015WE01 Nucl.Phys. A933, 114 (2015) D.Wei, L.Mao, N.Wang, M.Liu, L.Ou Further study on mechanism of production of light complex particles in nucleon-induced reactions NUCLEAR REACTIONS 27Al(p, d), (p, t), (p, 3He), (p, α), E=62 MeV;56Fe(n, d), (n, 3H), (n, 3He), (n, α), E=62, 175 MeV;58Ni(p, d), (p, t), (p, 3He), (p, α), E=1200 MeV;58Ni(p, p'), (p, n), (p, d), (p, t), (p, 3He), (p, α), E=175 MeV;63Cu(n, d), (n, 3H), E=317, 383, 477, 542 MeV;197Au(p, d), (p, t), (p, 3He), (p, α), E=1200 MeV; calculated σ(θ, Eout) using transport model and statistical model. Compared with available data.
doi: 10.1016/j.nuclphysa.2014.10.020
2015WU01 Phys.Rev. C 91, 014617 (2015) Q.h.Wu, Y.Zhang, Z.Xiao, R.Wang, Y.Zhang, Z.Li, N.Wang, R.H.Showalter Competition between Coulomb and symmetry potential in semi-peripheral heavy ion collisions NUCLEAR REACTIONS 197Au(40Ar, X), E=35, 50, 100 MeV/nucleon; calculated time evolution of the density contour plots, time evolution of symmetry potential for neutrons and protons, angular distribution of yields for neutrons and protons, correlation between symmetry energy and angular distribution of n/p ratios. Improved quantum molecular dynamics model (ImQMD05 code).
doi: 10.1103/PhysRevC.91.014617
2015ZH26 Phys.Rev. C 92, 024613 (2015) K.Zhao, Z.Li, N.Wang, Y.Zhang, Q.Li, Y.Wang, X.Wu Production mechanism of neutron-rich transuranium nuclei in 238U + 238U collisions at near-barrier energies NUCLEAR REACTIONS 238U(238U, X), E=7.0 MeV/nucleon; calculated isotopic production cross sections and most probable mass numbers of primary fragments and residual fragments with Z=78-106, A=180-280, 214Rn, 249,254,255,256Cf. Production of the light uranium-like and transuranium fragments. Improved quantum molecular dynamics (ImQMD) model incorporated with the statistical evaporation model using HIVAP code. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.024613
2014MO23 Phys.Rev. C 90, 024320 (2014) Systematic study of shell gaps in nuclei NUCLEAR STRUCTURE Z>8, N>8; analyzed S(2n), optimal values of the 18 independent model parameters, shell gaps using eight global nuclear mass models (FRDM, HFB17, HFB27, DZ28, WS, WS*, WS3, WS4), Weizsacker-Skyrme (WS4) mass formula based on measured and evaluated nuclear masses of 2353 nuclei in AME-2012. Magicity of N=184 from S(2n) and shell gaps, and shell closures in 208Pb and 270Hs. Magic numbers at Z=82 and 114. and subshell closures at Z=64, 92, 100, 120. No subshell closure at N=132 in Ra isotopes.
doi: 10.1103/PhysRevC.90.024320
2014TI04 Phys.Rev. C 90, 024313 (2014) J.Tian, H.Cui, K.Zheng, N.Wang Effect of Coulomb energy on the symmetry energy coefficients of finite nuclei NUCLEAR STRUCTURE A=10-270; calculated symmetry energy coefficients from differences between the masses of isobaric nuclei, using masses from AME-2012 for more than 2400 nuclei; deduced mass and Coulomb energy dependence on symmetry energy.
doi: 10.1103/PhysRevC.90.024313
2014WA07 Phys.Rev. C 89, 037601 (2014) Synthesis of superheavy nuclei with Z=118 in hot fusion reactions NUCLEAR REACTIONS 249,250,251,252Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E(cm)=190-260 MeV; 248Cm(50Ti, 2n), (50Ti, 3n), (50Ti, 4n), (50Ti, 5n), 244Pu(54Cr, 2n), (54Cr, 3n), (54Cr, 4n), (54Cr, 5n), E(cm)=200-280 MeV; calculated evaporation residue σ(E) for formation of Z=118 isotopes. Dinuclear system model with dynamical potential energy surface (DNS-DyPES model). Relevance to production of superheavy elements at JINR-Flerov Laboratory facility.
doi: 10.1103/PhysRevC.89.037601
2014WA22 Phys.Rev. C 89, 064601 (2014) Microscopic dynamics simulations of heavy-ion fusion reactions induced by neutron-rich nuclei NUCLEAR REACTIONS 76Ge(16O, X), E(cm)=30-50 MeV; 154Sm(16O, X), E(cm)=50-80 MeV; 96Zr(40Ca, X), E(cm)=85-120 MeV; 132Sn(40Ca, X), E=100-150 MeV; 92Zr(16O, X), E(cm)=37-60 MeV; 46Ti, 56Fe(16O, X), E(cm)=22-41 MeV; 58Ni(58Ni, X), E(cm)=90-120 MeV; 64Ni(64Ni, X), E(cm)=85-115 MeV; calculated fusion σ(E). 132Sn, 208Pb; calculated proton and neutron density distributions with time evolution. Improved quantum molecular dynamics (ImQMD) model with the parameter set SkP* and IQ3a. Comparison with theoretical calculations using Skyrme energy-density functional together with extended Thomas-Fermi (ETF2) approximation, and with experimental results.
doi: 10.1103/PhysRevC.89.064601
2014WA50 Phys.Rev. C 90, 054610 (2014) Systematic study of 16O-induced fusion with the improved quantum molecular dynamics model NUCLEAR REACTIONS 62Ni, 65Cu, 74Ge, 148Nd, 180Hf, 186W, 208Pb, 238U(16O, X), E(cm)=27-110 MeV; analyzed fusion σ(E) experimental data, density distribution contour for 186W+16O, charge distribution of fragments and momentum and density distribution in 16O+92Zr. improved quantum molecular dynamics (ImQMD) model with SkP* and IQ3a parameter sets.
doi: 10.1103/PhysRevC.90.054610
2014YE07 Phys.Rev. C 90, 041604 (2014) Probing nuclear dissipation with particle multiplicity in heavy-ion-induced light fissioning systems NUCLEAR STRUCTURE 200Pb, 251Es; calculated postsaddle multiplicities and change in binding energies of neutrons, protons, and α particles as a function of deformation parameter and angular momentum at excitation energy 120 MeV for 200Pb and 70 MeV for 251Es in the framework of Langevin models coupled to a statistical decay model.
doi: 10.1103/PhysRevC.90.041604
2014ZA07 Nucl.Phys. A929, 94 (2014) Temperature-dependent potential in alpha-decay process RADIOACTIVITY Pb, Po, Rn, Ra(α); calculated T1/2 for even-even isotopes. 220,227Th, 231Np, 246Es(α); calculated T1/2 vs temperature. A=150-266(α); calculated T1/2; deduced temperature of parent nuclei. Temperature dependent proximity potential.
doi: 10.1016/j.nuclphysa.2014.06.001
2014ZH24 Phys.Rev. C 90, 014303 (2014) J.S.Zheng, N.Y.Wang, Z.Y.Wang, Z.M.Niu, Y.F.Niu, B.Sun Mass predictions of the relativistic mean-field model with the radial basis function approach ATOMIC MASSES Z=8-100, N=8-170; calculated masses, S(2n), solar r-process abundances. Radial basis function (RBF) with relativistic mean-field (RMF) model. Comparison with experimental values from AME-2012.
doi: 10.1103/PhysRevC.90.014303
2013LI29 Phys.Rev. C 87, 064615 (2013) Finite-size effects on fragmentation in heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=15, 35, 45 MeV/nucleon; 197Au (197Au, X), E=15, 35, 60 MeV/nucleon; 129Sn(120Xe, X), E=39 MeV/nucleon; 48Ca(58Ni, X), E=25, 35 MeV/nucleon; calculated fragment charge distribution, average number of nucleons emitted from the ground states, isotopic yields. Influence of nuclear finite-size effects on fragmentation in heavy-ion collisions. Improved quantum molecular dynamics model (ImQMD). Comparison with experimental data.
doi: 10.1103/PhysRevC.87.064615
2013LI51 Chin.Phys.C 37, 114101 (2013) C.Li, J.-L.Tian, Y.-J.Qin, J.-J.Li, N.Wang Determination of the nucleon-nucleon interaction in the ImQMD model by nuclear reactions at the Fermi energy region NUCLEAR REACTIONS 40Ca(40Ca, X), E=10-45 MeV/nucleon; 120Sn(129Xe, X), E=32, 45 MeV/nucleon; 197Au(197Au, X), E=35, 50 MeV/nucleon; 197Au(238U, X), E=15 MeV/nucleon; calculated charge fragment distribution, multiplicity. Improved quantum molecular dynamic model.
doi: 10.1088/1674-1137/37/11/114101
2013TI01 Phys.Rev. C 87, 014313 (2013) Improved Kelson-Garvey mass relations for proton-rich nuclei ATOMIC MASSES 5Be, 6B, 13F, 15Ne, 18Mg, 16,17Na, 19,20,21,22Al, 21,22,23Si, 22,23,24,25,26P, 24,25,26,27S, 25,26,27,28,29,30Cl, 28,29,30,31,32,33,34K, 27,28,29,30,31Ar, 30,31,32,33,34,35Ca, 31,32,33,34,35,36,37,38Sc, 33,34,35,36,37,38,39Ti, 35,36,37,38,39,40,41,42,43V, 37,38,39,40,41,42,43,44,45Cr, 39,40,41,42,43,44,45,46,47Mn, 41,42,43,44,45,46,47,48,49Fe, 43,44,45,46,47,48,49,50,51,52Co, 45,46,47,48,49,50,51,52,53Ni, 47,48,49,50,51,52,53,54,55,56Cu, 49,50,51,52,53,54,55,56,57Zn, 60Ga, 62Ge, 64As, 66Se, 68Br, 70Kr, 72Rb, 74Sr; calculated binding energies, mass excess, Sp, S2p using improved Kelson-Garvey (ImKG) mass relations. Comparison with experimental data for mirror analogs. Predictions of masses for proton-rich nuclides. Discussed diproton emission.
doi: 10.1103/PhysRevC.87.014313
2013WA09 Phys.Rev. C 87, 034327 (2013) Nuclear symmetry energy from the Fermi-energy difference in nuclei NUCLEAR STRUCTURE 16,22O, 22,42Si, 40,48,60Ca, 42Ti, 56,68,78Ni, 130Cd, 100,132,134Sn, 134Te, 144Sm, 182,208Pb; calculated neutron-proton Fermi-energy difference, nuclear symmetry energy, neutron-skin thickness. Skyrme energy density functionals and nuclear masses, with 54 Skyrme parameter sets. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.034327
2013WA14 Phys.Rev. C 87, 051601 (2013) Exploring postsaddle nuclear dissipation with light-particle multiplicity at high energy NUCLEAR REACTIONS 232Th(19F, X)251Es*, E=100-140 MeV; 232Th (20Ne, X)252Fm*, E=215 MeV; 197Au(18O, X)215Fr*, E=159 MeV; 238U(18O, X)256Fm*, E=159 MeV; 208Pb(40Ar, X)248Fm*, E=249 MeV; 197Au(16O, X)213Fr*, E=288 MeV; 184W(16O, X)200Pb*, E=288 MeV; analyzed prescission neutron yields, and multiplicities of neutrons, protons, and α particles as function of postsaddle friction strength. Stochastic Langevin equation coupled with a statistical decay model.
doi: 10.1103/PhysRevC.87.051601
2013WA18 Phys.Rev. C 88, 011301 (2013) Shell and isospin effects in nuclear charge radii NUCLEAR STRUCTURE A>15, N=8-154; analyzed rms charge radii for 885 measured charge radii, and proposed a four-parameter phenomenological formula including shell correction and deformations from Weizsacker-Skyrme mass model and isospin dependent term. Comparison with HFB21 model calculations. Z=10-100; Z=20, N=18-32; Z=28, N=30-36; Z=40, N=46-62; Z=82, N=100-132; analyzed rms charge radii and compared with HFB21 and RMF model calculations. 30Si, 30S; analyzed nuclear symmetry energy, rms charge radii differences for mirror nuclei. A=254-310, Z=108, 112, 116, 120; predicted rms charge radii using the proposed formula, and compared with HFB21 model calculations.
doi: 10.1103/PhysRevC.88.011301
2013YE01 Phys.Rev. C 87, 014610 (2013) Significant role of level-density parameters in probing nuclear dissipation with light-ion-induced fission excitation functions NUCLEAR REACTIONS 197Au, 208Pb(3He, X), E*=50-150 MeV; analyzed fission σ(E), presaddle neutron probability. Bohr-Wheeler theory and Langevin approach.
doi: 10.1103/PhysRevC.87.014610
2013YE07 Phys.Rev. C 88, 054606 (2013) Roles of system size and excitation energy in probing nuclear dissipation with giant dipole resonance γ rays NUCLEAR STRUCTURE 200Pb, 224Th, 240Cf; calculated presaddle multiplicity of neutrons and GDR γ rays, multiplicities of postsaddle neutrons, protons and α particles, change of postsaddle GDR γ multiplicity Mγ as function of postsaddle friction β at different excitation energies of the fissioning system. Stochastic Langevin equation coupled to a statistical model of particle emission.
doi: 10.1103/PhysRevC.88.054606
2012JI07 Phys.Rev. C 85, 054303 (2012) H.Jiang, G.J.Fu, B.Sun, M.Liu, N.Wang, M.Wang, Y.G.Ma, C.J.Lin, Y.M.Zhao, Y.H.Zhang, Z.Ren, A.Arima Predictions of unknown masses and their applications ATOMIC MASSES Z=1-184, N=1-184; analyzed masses for 1566 nuclei using extrapolation approach and shell correction term, S(n), S(2n), S(p), and S(2p); one-neutron and one-proton drip nuclei, R-process nucleosynthesis and astrophysical implications. Comparison with AME-2011 interim mass evaluation, and with Duflo-Zuker model. 85Mo, 87,88,89Tc, 123Ag, 140I, 222Po, 226,227,228Rn, 233,234Ra, 235Ac; compared predicted masses with measured values. RADIOACTIVITY 248,249,250,251,252,253,254,255,256,257No, 251,252,253,254,255,256,257,258,259Lr, 253,254,255,256,257,258,259,260,261Rf, 255,256,257,258,259,260,261,262Db, 256,257,258,259,260,261,262,263Sg(α); calculated Q(α), half-life. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054303
2012QI08 Phys.Rev. C 85, 054623 (2012) Calculation of penetration probability across an arbitrary potential barrier in fusion reactions NUCLEAR REACTIONS 208Pb(18O, X), E=68-110 MeV; 90Zr(90Zr, X), E=190-210 MeV; calculated penetration probability, fusion σ(E), modified Bass potential barriers. Comparison with WKB (Wentzel-Kramers-Brillouin) approximation, Numerov calculations, and the transfer matrix approach. Double-hump barriers. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054623
2012SU01 Phys.Rev. C 85, 014613 (2012) Pre-neutron-emission mass distributions for low-energy neutron-induced actinide fission NUCLEAR REACTIONS 235,238U, 237Np, 232Th, 239Pu(n, F), E=0.3-6 MeV; calculated pre-neutron-emission mass distributions, driving potential, phenomenological fission potential, energy dependence of the potential parameters, effect of nuclear deformations on potential parameters. Skyrme energy-density functional. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014613
2012WA12 Phys.Rev. C 85, 041601 (2012) N.Wang, E.-G.Zhao, W.Scheid, S.-G.Zhou Theoretical study of the synthesis of superheavy nuclei with Z=119 and 120 in heavy-ion reactions with trans-uranium targets NUCLEAR REACTIONS 238U, 237Np, 242Pu, 243Am, 248Cm, 249Bk, 249Cf(48Ca, xn)283Cn/282Nh/286Fl/288Mc/292Lv/293Ts/294Og, E(cm)=194.7-211.3 MeV; 249Bk, 249,251Cf(50Ti, xn)295119/296120/298120, E(cm)=220-280 MeV; calculated maximal values of evaporation-residue cross sections. Dinuclear system model with a dynamical potential energy surface (DNS-DyPES). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.041601
2012YE08 Phys.Rev. C 86, 034605 (2012) Robustness of the excitation energy at scission as a novel probe of nuclear dissipation at high energy NUCLEAR STRUCTURE 194,200,206Hg, 200Rn, 240Cf; calculated excitation energy of compound nuclei at scission, evaporated multiplicities of prescission neutrons, protons and α particles, fission barriers, emission barriers of protons and α particles of the fissioning systems. Langevin model with statistical description of particle evaporation from fissioning compound nuclei.
doi: 10.1103/PhysRevC.86.034605
2012ZA02 Phys.Rev. C 85, 034601 (2012) V.Zanganeh, N.Wang, O.N.Ghodsi Dynamical nucleus-nucleus potential and incompressibility of nuclear matter NUCLEAR REACTIONS 208Pb(48Ca, X), E(cm)=179, 200, 205 MeV; calculated time evolution of density distribution, dynamical nucleus-nucleus potential, nuclear potential. 208Pb(16O, X), E(cm)=70-110 MeV; calculated fusion excitation function, dynamical nucleus-nucleus potential. 197Au(197Au, X), 40Ca(40Ca, X), E=35 MeV/nucleon; calculated fragment charge distribution. Improved quantum molecular-dynamics (ImQMD) model using several interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034601
2012ZH02 Phys.Rev. C 85, 014325 (2012) H.F.Zhang, Y.Gao, N.Wang, J.Q.Li, E.G.Zhao, G.Royer Double magic nuclei for Z>82 and N>126 NUCLEAR STRUCTURE Z=101-118, N=140-194; calculated binding energies, Q(α). Z=101-129, N=162, 184; calculated S(p), Q(α) using Macroscopic-microscopic model (MMM). 270Hs, 298Fl; calculated potential energy in the constrained relativistic mean-field (CRMF) theory with effective interaction NL3. Comparison with experimental data. RADIOACTIVITY 269Sg, 274Bh, 273Hs, 278Mt, 277,281Ds, 282Rg, 281,285Cn, 285,286Nh, 285,288,289Fl, 289,290Mc, 293,294Ts(α); Z=108, N=148-172(α); Z=114, N=160-190(α); calculated α decay half-lives. Macroscopic-microscopic model (MMM). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014325
2011DO19 Chin.Phys.Lett. 28, 122401 (2011) Nuclear Dynamical Quadrupole Deformations in Heavy-Ion Reactions NUCLEAR REACTIONS 48Ca(40Ca, X), E(cm)=60 MeV; 90Zr(40Ca, X), E(cm)=108 MeV; calculated quadrupole deformations and energies for projectile and target nuclei; deduced prolate deformation parameters. Quantum molecular dynamics model.
doi: 10.1088/0256-307X/28/12/122401
2011LI31 Phys.Rev. C 84, 014333 (2011) Further improvements on a global nuclear mass model ATOMIC MASSES A=1-240; analyzed deviations of calculated nuclear masses total g.s. energies, and S(n) from the experimental data, b coefficients of nuclei in the IMME as a function of mass number. A=260-320; calculated Q(α). Global nuclear mass models. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.014333
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
2011WA38 Phys.Rev. C 84, 051303 (2011) Nuclear mass predictions with a radial basis function approach ATOMIC MASSES A=16-264; analyzed masses, rms deviation from recommended values for 2149 nuclei, S(n) values. Radial basis function (RBF) and the Garvey-Kelson relation with global nuclear mass models. The AME95-03 and AME03-Border tests.
doi: 10.1103/PhysRevC.84.051303
2011WA41 Phys.Rev. C 84, 061601 (2011) Systematics of fusion probability in "hot" fusion reactions NUCLEAR REACTIONS 238U, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 3n), (48Ca, 4n), E(cm)=190-220 MeV; 208Pb(48Ca, n), (48Ca, 2n), E(cm)=160-200 MeV; 208Pb(50Ti, n), (50Ti, 2n), E(cm)=170-210 MeV; 208Pb(54Cr, n), (54Cr, n), E(cm)=195-220 MeV; 208Pb(58Fe, n), (58Fe, 2n), E(cm)=210-230 MeV; 209Bi(58Fe, n), E(cm)=210-230 MeV; 208Pb(62Ni, n), E(cm)=235-255 MeV; 208Pb(64Ni, n), E(cm)=235-255 MeV; 208Pb(70Zn, n), E(cm)=250-270 MeV; 209Bi(64Ni, n), E(cm)=235-260 MeV; 209Bi(70Zn, n), E(cm)=255-270 MeV; 249Bk(50Ti, 3n), (50Ti, 4n), E(cm)=210-240 MeV; 248Cm(54Cr, 3n), (54Cr, 4n), E(cm)=230-255 MeV; 249Cf(50Ti, 3n), (50Ti, 4n), E(cm)=215-245 MeV; 244Pu(58Fe, 3n), (58Fe, 4n), E(cm)=240-270 MeV; calculated evaporation residual cross sections. Hot fusion reactions, super-heavy nuclei. Skyrme energy-density functionals. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.061601
2010JI05 Phys.Rev. C 81, 044602 (2010) Y.Jiang, N.Wang, Z.Li, W.Scheid Dynamical nucleus-nucleus potential at short distances NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=50-140 MeV; 208Pb(48Ca, X), E(cm)=170-210 MeV; 130Te(126Sn, X), E(cm)=270-360 MeV; calculated σ(E), nucleus-nucleus potentials, barrier heights, particle kinetic energy using improved quantum molecular dynamics (ImQMD) model together with the extended Thomas-Fermi (ETF) approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044602
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
2010WA09 Phys.Rev. C 81, 044322 (2010), Publishers Note Phys.Rev. C 81, 059902 (2010) Modification of nuclear mass formula by considering isospin effects NUCLEAR STRUCTURE 16O, 48Ca, 208Pb; calculated energies, β2 and β4 deformation parameters. 82Sr; calculated potential energy surface as function of β2 and β4 deformation parameters. 16,24O, 40,48Ca, 90Zr, 132Sn, 208Pb, 270Hs, 288,290,292,294116, N=2-240; calculated shell corrections. Skyrme energy-density functional approach. Comparison with experimental data. ATOMIC MASSES Z=10-130, N=10-230; calculated nuclear masses for 2149 nuclei using Skyrme energy-density functional approach and comparison with FRDM and HFB-17 results. Comparison with experimental data. Semiempirical nuclear mass formula based on the macroscopic-microscopic method with Woods-Saxon density distribution.
doi: 10.1103/PhysRevC.81.044322
2010WA15 Chin.Phys.Lett. 27, 062502 (2010) N.Wang, L.Dou, E.-G.Zhao, W.Scheid Nuclear Hexadecapole Deformation Effects on the Production of Super-Heavy Elements NUCLEAR REACTIONS 209Bi(58Fe, X)267Mt, 208Pb(64Ni, X)272Ds, 209Bi(70Zn, X)279Nh, 209Bi(74Ge, X)283Mc, 208Pb(86Se, X)294Lv, 208Pb(90Kr, X)298Og, E not given; calculated interaction and driving potentials, fusion probabilities; deduced impact of nuclear hexadecapole deformation for production of super-heavy elements.
doi: 10.1088/0256-307X/27/6/062502
2010WA24 Phys.Rev. C 81, 067302 (2010) Mass and isospin dependence of symmetry energy coefficients of finite nuclei NUCLEAR STRUCTURE A=1-250; analyzed symmetry-energy coefficients as a function of nuclear mass number and isospin asymmetry., Wigner energies using the liquid drop mass formula and measured nuclear masses.
doi: 10.1103/PhysRevC.81.067302
2010WA28 Nucl.Phys. A834, 212c (2010) Extraction of probability of compound-nucleus formation NUCLEAR STRUCTURE Z=102-118; compiled, analyzed capture σ, probability of compound nucleus formation. Comparison with other data.
doi: 10.1016/j.nuclphysa.2009.12.043
2010WA38 Phys.Rev. C 82, 044304 (2010) Mirror nuclei constraint in nuclear mass formula ATOMIC MASSES Z>8, N>8; analyzed model parameters of the semiempirical mass formula using measured masses of 2149 nuclei with mirror nuclei constraints, shell corrections, contour plots of β2, β4 and β6 deformation parameters as a function of neutron number, neutron drip lines, fission barriers of SHE, Q(α) values. Prediction of central region of SHE near N=176-178 and Z=116-120.
doi: 10.1103/PhysRevC.82.044304
2008WA01 Phys.Rev. C 77, 014603 (2008) N.Wang, K.Zhao, W.Scheid, X.Wu Fusion-fission reactions with a modified Woods-Saxon potential RADIOACTIVITY 256No(SF); calculated macroscopic fission barrier. NUCLEAR REACTIONS 113,115In(7Li, X), E(cm)=18-36 MeV; 108,110Pd(12C, X), E(cm)=32-50 MeV; 194,198Pt(12C, X), E(cm)=50-70 MeV; 197Au(12C, X), E(cm)=45-105 MeV; 208Pb(12C, X), E(cm)=50-70 MeV; 182,186W(16O, X), E(cm)=60-90 MeV; 197Au(16O, X), E(cm)=70-120 MeV; 208Pb(16O, X), E(cm)=65-100 MeV; 169Tm, 181Ta, 197Au, 208Pb(19F, X), E(cm)=60-120 MeV; 192Os(18O, X), E(cm)=70-110 MeV; 197Au(18O, X), E(cm)=60-120 MeV; 238U(16O, X), E(cm)=60-110 MeV; 154Sm(48Ca, X), E(cm)=120-165 MeV; 92Zr(64Ni, X), E(cm)=120-180 MeV; 112,118,124Sn(64Ni, X), E(cm)=150-200 MeV; 186W(30Si, X), E(cm)=100-160 MeV; 176Er(30Si, X), E(cm)=100-150 MeV; 208Pb(28Si, X), E(cm)=115-165 MeV; 70,76Ge(86Kr, X), E(cm)=120-180 MeV; 92Mo(86Kr, X), E(cm)=150-190 MeV; 144,148,154Sm(40Ar, X), E(cm)=105-145 MeV; 112,120Sn(35Cl, X), E(cm)=100-130 MeV; 141Pr(35Cl, X), E(cm)=110-140 MeV; 112,116,122Sn(40Ar, X), E(cm)=90-130 MeV; 248Cm(18O, X), E(cm)=80-105 MeV; 206Pb(48Ca, X), E(cm)=165-200 MeV; 207,208Pb(48Ca, X), E(cm)=165-195 MeV; 208Pb(50Ti, X), E(cm)=180-210 MeV; 208Pb(54Cr, X), E(cm)=200-215 MeV; 208Pb(58Fe, X), E(cm)=215-225 MeV; 208Pb(64Ni, X), E(cm)=235-245 MeV; calculated neutron evaporation cross sections using Woods-Saxon potentials. A=0-300; calculated level density parameter.
doi: 10.1103/PhysRevC.77.014603
2008WA02 Chin.Phys.Lett. 25, 77 (2008) Shell Correction and Pairing Energies in the Dinuclear System Model NUCLEAR REACTIONS 208Pb(76Ge, X), (86Kr, X), E not given; calculated fusion probabilities, compound nuclei survival probability, and evaporation residue cross sections.
doi: 10.1088/0256-307X/25/1/022
2008WA16 Phys.Rev. C 78, 014607 (2008) Quasi-elastic scattering and fusion with a modified Woods-Saxon potential NUCLEAR REACTIONS 208Pb(12C, 12C'), E=69.9, 74.9, 84.9, 180 MeV;208Pb(16O, 16O'), E=92, 96, 102, 192 MeV;90Zr(12C, 12C'), E=100, 120, 180 MeV;63Cu(16O, 16O'), E=56, 64, 100 MeV; calculated quasi-elastic scattering σ. 232Th(16O, 16O'), E(cm)=74-100 MeV; calculated transfer probability, fusion excitation factors. 144,154Sm(16O, 16O), E(cm)=45-75;92Zr(16O, 16O), E(cm)=30-60 MeV;186W(16O, 16O'), E=50-90 MeV;116Sn(16O, 16O'), E(cm)=35-70 MeV;64Zn(16O, 16O'), E(cm)=20-45 MeV;232Th(16O, 16O), E(cm)=60-100 MeV;142Nd(12C, 12C'), E(cm)=35-60 MeV;208Pb(32S, 32S'), E(cm)=120-180 MeV;110Pd(32S, 32S'), E(cm)=70-110 MeV; calculated fusion σ, scattering σ. Woods-Saxon model. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.014607
2008WA20 Phys.Rev. C 78, 054607 (2008) Orientation effects of deformed nuclei on the production of superheavy elements NUCLEAR REACTIONS 208Pb(58Fe, X), (70Zn, X), (82Se, X), (86Kr, X), E=10-18 MeV; calculated potential energy surfaces, interaction potentials, σ, fission barriers. Dinuclear system model.
doi: 10.1103/PhysRevC.78.054607
2008ZH27 Int.J.Mod.Phys. E17, 1937 (2008) E.G.Zhao, N.Wang, Z.Q.Feng, J.Q.Li, S.G.Zhou, W.Scheid The isotopic and nuclear orientation effects on the production of super-heavy elements NUCLEAR REACTIONS 208Pb(48Ca, X), (56Fe, X), (70Zn, X), (82Se, X), (86Kr, X), E not given; 236,237,238,239,240,241,242,243,244Pu(48Ca, X), E not given; calculated fusion evaporation cross sections for super heavy element formations.
doi: 10.1142/S021830130801091X
2007FE12 Chin.Phys.Lett. 24, 2551 (2007) Z.-Q.Feng, G.-M.Jin, M.-H.Huang, Z.-G.Gan, N.Wang, J.-Q.Li Possible Way to Synthesize Superheavy Element Z = 117 NUCLEAR REACTIONS 247,248,249Bk(48Ca, xn), 246Cm(45Sc, xn), 244Pu(51V, xn), 238U(55Mn, xn), 232Th(59Co, xn), 209Bi(76Se, n), (77Se, n), (78Se, n), (79Se, n), (80Se, n), (82Se, n), e not given; calculated cross sections and evaporation residue excitation functions within the framework of the dinuclear system model.
doi: 10.1088/0256-307X/24/9/024
2007HU22 Chin.Phys.Lett. 24, 2792 (2007) Y.-S.Huang, N.-Y.Wang, X.-J.Duan, X.-F.Lan, Z.-X.Tan, X.-Z.Tang, Y.-X.Ye Neutron Generation and Kinetic Energy of Expanding Laser Plasmas
doi: 10.1088/0256-307X/24/10/022
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
2007WA23 Chin.Phys.Lett. 24, 2219 (2007) N.Wang, J.-Q.Li, E.-G.Zhao, Z.-Q.Feng Nuclear Potential and Fusion Cross Sections for Synthesizing Super-Heavy Elements in Di-nuclear Systems NUCLEAR REACTIONS 208Pb(54Cr, X), (58Fe, X), (64Ni, X), (82Se, X), E not given; calculated interaction potentials, fusion probability and evaporation residue cross sections using a double folding method with simplified Skyrme type nucleon-nucleon interaction.
doi: 10.1088/0256-307X/24/8/018
2006LI09 Nucl.Phys. A768, 80 (2006) M.Liu, N.Wang, Z.Li, X.Wu, E.Zhao Applications of Skyrme energy-density functional to fusion reactions spanning the fusion barriers NUCLEAR REACTIONS 92Zr(12C, X), E(cm) ≈ 24-48 MeV; 70,72,73,74,76Ge, 92Zr, 112Cd, 144Nd, 144,147,148,149,150,154Sm, 166Er, 186W, 208Pb, 232Th(16O, X), E(cm) ≈ 30-160; 144Sm(17O, X), E(cm) ≈ 50-100 MeV; 197Au, 208Pb(19F, X), E(cm) ≈ 70-150 MeV; 70,72,73,74,76Ge(27Al, X), E(cm) ≈ 45-65 MeV; 28Si, 92Zr, 178Hf(28Si, X), E(cm) ≈ 20-150 MeV; 186W(30Si, X), E(cm) ≈ 105-165 MeV; 175Lu(31P, X), E(cm) ≈ 100-150 MeV; 154Sm, 181Ta, 182W(32S, X), E(cm) ≈ 120-200 MeV; 90,92Zr(33S, X), E(cm) ≈ 70-100 MeV; 54Fe, 92Zr(35Cl, X), E(cm) ≈ 50-100 MeV; 90Zr(50Ti, X), E(cm) ≈ 90-130 MeV; 64Ni(132Sn, X), E(cm) ≈ 140-180 MeV; analyzed fusion excitation functions, fusion barrier features. Extended semi-classical Thomas-Fermi method, suppression and enhancement effects discussed.
doi: 10.1016/j.nuclphysa.2006.01.011
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
Back to query form [Next] Note: The following list of authors and aliases matches the search parameter N.Wang: , N.W.WANG, N.Y.WANG |