NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Su Found 135 matches. Showing 1 to 100. [Next]2024GA08 Phys.Rev. C 109, 024601 (2024) Z.Gao, S.Liu, P.Wen, Z.Liao, Y.Yang, J.Su, Y.Wang, L.Zhu Constraining the Woods-Saxon potential in fusion reactions based on the neural network
doi: 10.1103/PhysRevC.109.024601
2024HU04 Phys.Rev. C 109, 034609 (2024) Y.G.Huang, F.C.Gu, Y.J.Feng, H.Wang, E.X.Xiao, X.Lei, L.Zhu, J.Su Multimodality of 187Ir fission studied by the Langevin approach
doi: 10.1103/PhysRevC.109.034609
2024XI03 Chin.Phys.C 48, 014104 (2024) E.Xiao, X.Lei, Y.Huang, Y.Feng, L.Zhu, J.Su Uncertainties of critical temperatures based on higher-order fluctuations of the largest fragment charge NUCLEAR REACTIONS 40Ca, 56Fe, 90Zr, 120Sn, 136Xe, 197Au(124Sn, X), E=400-1000 MeV/nucleon; analyzed available data; deduced parameters from the isotope thermometer utilizing the isospin-dependent quantum molecular dynamics model in conjunction with the statistical model GEMINI; deduced new signature of liquid-gas phase transition.
doi: 10.1088/1674-1137/ad021d
2023DU05 Eur.Phys.J. A 59, 93 (2023) H.-X.Duan, F.Zhang, J.Su, L.Zhu, C.-C.Guo Studying sub-saturation density symmetry energy with different nuclear thermometers NUCLEAR REACTIONS U(155Gd, X), E not given; 197Au(197Au, X), E=35 MeV/nucleon; analyzed available data; deduced the relation between nuclear temperatures and symmetry energy using the IQMD model.
doi: 10.1140/epja/s10050-023-01008-5
2023FE04 Phys.Rev. C 107, 044606 (2023) Y.Feng, Y.Huang, E.Xiao, X.Lei, L.Zhu, J.Su Contributions of quasifission and fusion-fission in the 24Mg + 178Hf reaction at 145 MeV laboratory beam energy using the Boltzmann-Uehling-Uhlenbeck model NUCLEAR REACTIONS 178Hf(24Mg, X), E=145 MV/nucleon; calculated time evolution of dinuclear systems of two fragments, mass numbers of fragment pairs, change of distance between fragments over time, σ of total capture, quasifission and fusion, contribution of quasi-inelastic, quasifission and fusion processes, mass-angular correlation of the fragments, dependence of the σ on the incompressibility parameter. Boltzmann-Uehling-Uhlenbeck model used with phase-space-density constraint (PSDC) method to describe heavy-ion collision near the Coulomb barrier. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.044606
2023LE01 Chin.Phys.C 47, 014102 (2023) X.Lei, E.Xiao, Y.Feng, Y.Huang, L.Zhu, J.Su Production of neutron-deficient nuclei around N = 126 by proton-induced spallation NUCLEAR REACTIONS 237Np, 239Pu, 241Am, 243Cm, 247Bk, 252Cf(p, X), E=1 GeV; analyzed available data. 217,218,221Np, 222,223,224,225,226,227Pu, 225,226,227,228,231Am; deduced σ, yields. Comparison with the IQMD-GEMINI++ model calculations.
doi: 10.1088/1674-1137/ac9601
2023LI08 Phys.Rev. C 107, 014614 (2023) Dynamics of charge equilibration and effects on producing neutron-rich isotopes around N = 126 in multinucleon transfer reactions NUCLEAR REACTIONS 198Pt(129Xe, X), E(cm)=470; 198Pt(136Xe, X), E(cm)=476 MeV; (140Xe, X), E(cm)=466 MeV; calculated average N/Z values of projectile-like (PLF) and target-like (TLF) fragments as a function of the contact time, production σ for N=126 isotones. 198Pt(140Xe, X), (202Pt, X), (238U, X), E(cm)=466, 663, 741 MeV; calculated σ production of Ta, Re, W, and Os isotopes. Extended version of the dinuclear system model and the improved quantum molecular dynamics (ImQMD) model.
doi: 10.1103/PhysRevC.107.014614
2023LI11 Phys.Rev. C 107, 024609 (2023) G.-S.Li, J.Su, B.-H.Sun, S.Terashima, J.-W.Zhao, X.-D.Xu, J.-C.Zhang, G.Guo, L.-C.He, W.-P.Lin, W.-J.Lin, C.-Y.Liu, C.-G.Lu, B.Mei, Z.-Y.Sun, I.Tanihata, M.Wang, F.Wang, S.T.Wang, X.-L.Wei, J.Wang, J.-Y.Xu, J.-R.Liu, M.-X.Zhang, Y.Zheng, L.-H.Zhu, X.-H.Zhang New measurement of the elemental fragmentation cross sections of 218 MeV/nucleon 28Si on a carbon target NUCLEAR REACTIONS 12C(28Si, X), E=218 MeV/nucleon; measured reaction products, time-of-flight; deduced charge changing σ, elemental fragmentation σ (EFCSs) with charge changes 1-6. Comparison to the previous measurements and to the predictions from the models EPAX2, EPAX3, FRACS, ABRABLA07, NUCFRG2, and IQMD coupled with GEMINI (IQMD+GEMINI). Particle identification by means of MWPC and MUSIC detectors. Beam of 28Si produced from 9Be(40Ar, X), E=320 MeV/nucleon at Heavy Ion Research Facility (HIRFL-CSR, Lanzhou).
doi: 10.1103/PhysRevC.107.024609
2023LI29 Phys. Rev. Res. 5, L022021 (2023) Z.Liao, L.Zhu, Z.Gao, J.Su, C.Li Optimal detection angles for producing N=126 neutron-rich isotones in multinucleon transfer reactions NUCLEAR REACTIONS 208Pb(136Xe, X)204Pt/203Ir/202Os/201Re, E(cm)=526 MeV; calculated optimal angle ranges for detecting N=126 neutron-rich nuclides in the multinucleon transfer (MNT) process.
doi: 10.1103/PhysRevResearch.5.L022021
2023SH06 Astrophys.J. 945, 41 (2023) Y.Shen, B.Guo, R.J.deBoer, E.Li, Z.Li, Y.Li, X.Tang, D.Pang, S.Adhikari, C.Basu, J.Su, S.Yan, Q.Fan, J.Liu, C.Chen, Z.Han, X.Li, G.Lian, T.Ma, W.Nan, W.Nan, Y.Wang, S.Zeng, H.Zhang, W.Liu New Determination of the 12C(α, γ)16O Reaction Rate and Its Impact on the Black-hole Mass Gap NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; measured reaction products. 16O; deduced σ(θ), the asymptotic normalization coefficient (ANC) for the 16O ground state (GS), astrophysical S-factor and the stellar rate. The HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE) in Beijing, China.
doi: 10.3847/1538-4357/acb7de
2023SO06 Phys.Rev. C 107, 044609 (2023) Q.Song, L.Zhu, B.Cai, C.Yuan, J.Su, H.Guo Image processing of isotope yield in neutron-induced fission NUCLEAR REACTIONS 235U, 229Th(n, F), E=2 MeV;243Am, 236,238Np(n, F), E=0.0253 eV;239Pu(n, F), E=0.5 MeV; calculated fission yield mass distribution, fragments isomeric ratios for 128Sb, 130Sb, 132Sb, 131Te, 133Te, 132I, 134I, 133Xe, 135Xe. Predictions of machine-learning algorithm based on tensor decomposition method trained on 851 fission products from ENDF/ B-VIII.0 database. Comparison experimental data, TALYS and GEF calculations and JEFF-3.3, ENDF/B-VIII.0 evaluations.
doi: 10.1103/PhysRevC.107.044609
2023WA05 Phys.Rev.Lett. 130, 092701 (2023) L.H.Wang, J.Su, Y.P.Shen, J.J.He, M.Lugaro, B.Szanyi, A.I.Karakas, L.Y.Zhang, X.Y.Li, B.Guo, G.Lian, Z.H.Li, Y.B.Wang, L.H.Chen, B.Q.Cui, X.D.Tang, B.S.Gao, Q.Wu, L.T.Sun, S.Wang, Y.D.Sheng, Y.J.Chen, H.Zhang, Z.M.Li, L.Y.Song, X.Z.Jiang, W.Nan, W.K.Nan, L.Zhang, F.Q.Cao, T.Y.Jiao, L.H.Ru, J.P.Cheng, M.Wiescher, W.P.Liu Measurement of the 18O(α, γ)22Ne Reaction Rate at JUNA and Its Impact on Probing the Origin of SiC Grains NUCLEAR REACTIONS 18O(α, γ), E=470-787 keV; measured reaction products, Eγ, Iγ; deduced thick target yields, resonance energies and resonance strengths, total reaction rates. Comparison with available data. The Jinping Underground Nuclear Astrophysics experimental facility (JUNA).
doi: 10.1103/PhysRevLett.130.092701
2023ZH26 Phys.Rev. C 107, 065801 (2023) H.Zhang, J.Su, Z.H.Li, Y.J.Li, E.T.Li, C.Chen, J.J.He, Y.P.Shen, G.Lian, B.Guo, X.Y.Li, L.Y.Zhang, Y.D.Sheng, Y.J.Chen, L.H.Wang, L.Zhang, F.Q.Cao, W.Nan, W.K.Nan, G.X.Li, N.Song, B.Q.Cui, L.H.Chen, R.G.Ma, Z.C.Zhang, T.Y.Jiao, B.S.Gao, X.D.Tang, Q.Wu, J.Q.Li, L.T.Sun, S.Wang, S.Q.Yan, J.H.Liao, Y.B.Wang, S.Zeng, D.Nan, Q.W.Fan, W.P.Liu Updated reaction rate of 25Mg(p, γ)26Al and its astrophysical implication NUCLEAR REACTIONS 25Mg(p, γ), E=117-350 keV; measured Eγ, Iγ, sum of γ energies; deduced γ-ray branching ratios, resonances, resonance strengths, astrophysical reaction rate (T=0.01-2.0 GK), contribution of individual resonances to the reaction rate, ground-state and isomeric state contribution. Comaprison to other experimental data and NACRE compilation. Evaluated the impact of the obtained data on the 26Al yield in stellar environment (code MESA). BGO detector array in nearby 4π geometry composed of 8 identical segments at high-current 400 kV JUNA accelerator (China JinPing underground Laboratory).
doi: 10.1103/PhysRevC.107.065801
2022HU06 Phys.Lett. B 831, 137183 (2022) H.Hu, W.-L.Guo, J.Su, W.Wang, C.Yuan Implementation of residual nucleus de-excitations associated with proton decays in 12C based on the GENIE generator and TALYS code RADIOACTIVITY 12C(p); analyzed available dat. 11B, 10B, 10Be; calculated de-excitation processes of residual nuclei associated with proton decays in based on the GENIE generator and TALYS code.
doi: 10.1016/j.physletb.2022.137183
2022HU20 Phys.Rev. C 106, 054606 (2022) Y.Huang, Y.Feng, E.Xiao, X.Lei, L.Zhu, J.Su Influence of pre-scission neutron emission on high-energy 238U fission studied by the Langevin approach NUCLEAR REACTIONS 238U(n, F), E=110, 325, 500 MeV; calculated potential energy surfaces, Langevin trajectory, pre-scission neutron multiplicity and kinetic energy, fragment mass distributions, average fragment mass, total kinetic energy of fission fragments, fragment deformation distribution. Three-dimensional Langevin approach considering nucleus elongation, deformation, and mass asymmetry coupled with Hauser-Feshbach statistical decay model to simulate the pre-scission neutron emission. Comparison with experimental data.
doi: 10.1103/PhysRevC.106.054606
2022LI28 Few-Body Systems 63, 43 (2022) W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho Progress of Underground Nuclear Astrophysics Experiment JUNA in China NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.
doi: 10.1007/s00601-022-01735-3
2022LI47 Phys.Rev. C 106, 025807 (2022) X.Y.Li, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, J.J.He, S.Q.Yan, Q.W.Fan, J.C.Liu, L.Gan, Z.Y.Han, E.T.Li, G.Lian, Y.P.Shen, Y.B.Wang, S.Zeng, W.P.Liu Astrophysical 15N(n, γ)16N reaction rate from precision measurement of the 15N(d, p)16N angular distributions NUCLEAR REACTIONS 15N(d, p), (d, d), E=15 MeV; measured particle spectra, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA and ADWA analysis. 15N(n, γ), T=0.01-10 GK; deduced astrophysical reaction rates; calculated σ(E). Comparison with previous experimental results, and with OXBASH shell-model predictions.
doi: 10.1103/PhysRevC.106.025807
2022LI72 Phys.Rev. C 106, 065804 (2022) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, D.X.Wang, S.Y.Zhang, G.L.Yang, X.K.Li, Z.D.An, J.J.He, W.Luo, X.G.Cao, L.L.Song, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, Y.D.Liu, C.W.Ma, Y.T.Wang, J.Su, L.Y.Zhang, Y.X.Yang, S.Feng, W.B.Liu, W.Q.Su, S.Jin, K.J.Chen Experimental determination of the neutron resonance peak of 162Er at 67.8 eV NUCLEAR REACTIONS 162Er(n, γ), E=20-100 eV; measured Eγ, Iγ; deduced neutron-capture yield, resonances, decay widths. Resonance parameters at 67.8 eV are extracted for the first time. R-matrix analysis. Comparison to other experimental results and ENDF/B-VIII.0 data. 4 C6D6 detectors. Neutron beam from Back-n Facility of the CSNS.
doi: 10.1103/PhysRevC.106.065804
2022SO09 Chin.Phys.C 46, 074108 (2022) Target dependence of isotopic cross sections in the spallation reactions 238U + p, d and 9Be at 1 AGeV NUCLEAR REACTIONS 1,2H, 9Be(238U, X), E=1 GeV/nucleon; calculated spallation σ using physical model dependent (Bayesian neural network) BNN, which includes the details of IQMD-GEMINI++ model and BNN.
doi: 10.1088/1674-1137/ac6249
2022SU05 Phys.Rev. C 105, 024608 (2022) Fluctuations of the largest fragment charge in projectile fragmentation and its nonequilibrium effect NUCLEAR REACTIONS 120Sn(124Sn, X), E=600 MeV/nucleon; calculated fluctuations of the largest fragment charge, mean multiplicity of intermediate-mass fragments for the equilibrium and nonequilibrium systems. Isospin-dependent quantum molecular dynamics (IQMD) model calculations. Comparison with available data.
doi: 10.1103/PhysRevC.105.024608
2022WA02 Nucl.Instrum.Methods Phys.Res. B512, 49 (2022) L.H.Wang, Y.P.Shen, J.Su, X.Y.Li, W.Q.Yan, J.J.He, L.Y.Zhang, B.Liao, Y.F.Wu, Y.D.Sheng, Z.M.Li, Y.J.Chen, L.Y.Song, X.Z.Jiang, G.Lian, W.Nan, W.K.Nan, L.Zhang, F.Q.Cao, C.Chen, N.Song, H.Zhang, W.P.Liu Development of irradiation-resistant enriched 12C targets for astrophysical 12C(α, γ)16O reaction measurements NUCLEAR REACTIONS 12C(p, γ), E=370 keV; 12C(p, α), E=740 keV; measured reaction products, Eγ, Iγ; deduced yields. The China JinPing underground Laboratory (CJPL).
doi: 10.1016/j.nimb.2021.11.020
2022XI03 J.Phys.(London) G49, 065102 (2022) E.Xiao, Y.Feng, X.Lei, L.Zhu, J.Su Dissipation of energy and higher-order fluctuations of the largest fragment charge in projectile fragmentation NUCLEAR REACTIONS 120Sn(107Sn, X), E=60 MeV/nucleon; calculated density of the participant center, collective velocity, correlations between impact parameters, mean multiplicity of IMF. The isospin-dependent quantum molecular dynamics (IQMD) model is used to study the non-equilibrium thermalization and fragmentation.
doi: 10.1088/1361-6471/ac4f28
2022ZH60 Nature(London) 610, 656 (2022) L.Zhang, J.He, R.J.deBoer, M.Wiescher, A.Heger, D.Kahl, J.Su, D.Odell, Y.Chen, X.Li, J.Wang, L.Zhang, F.Cao, H.Zhang, Z.Zhang, X.Jiang, L.Wang, Z.Li, L.Song, H.Zhao, L.Sun, Q.Wu, J.Li, B.Cui, L.Chen, R.Ma, E.Li, G.Lian, Y.D.Sheng, Z.Li, B.Guo, X.Zhou, Y.Zhang, H.Xu, J.Cheng, W.Liu Measurement of 19F(p, γ)20Ne reaction suggests CNO breakout in first stars NUCLEAR REACTIONS 19F(p, γ), E(cm)<400 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factor, resonance strengths, astrophysical reaction rates. Comparison with available data. The Jinping Underground Nuclear Astrophysics Experiment (JUNA).
doi: 10.1038/s41586-022-05230-x
2022ZH67 Phys.Rev. C 106, 055803 (2022) L.Y.Zhang, J.Su, J.J.He, R.J.deBoer, D.Kahl, M.Wiescher, D.Odell, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, B.Guo, X.D.Tang, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, J.P.Cheng, W.P.Liu Direct measurement of the astrophysical 19F(p, αγ)16O reaction in a deep-underground laboratory NUCLEAR REACTIONS 19F(p, αγ), E(cm)=72.4-344 keV; measured Eγ, Iγ; deduced astrophysical S-factor, thermonuclear astrophysical reaction rates (range 0.05–1 GK), contributions from different channels. R-matrix analysis with AZURE2 together with a MCMC Bayesian uncertainty estimation. Comparison to other experimental data. 4π BGO γ-array with proton beam from JUNA accelerator at China JinPing underground Laboratory (CJPL).
doi: 10.1103/PhysRevC.106.055803
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
2021HU23 Phys.Rev.Lett. 127, 172701 (2021) J.Hu, H.Yamaguchi, Y.H.Lam, A.Heger, D.Kahl, A.M.Jacobs, Z.Johnston, S.W.Xu, N.T.Zhang, S.B.Ma, L.H.Ru, E.Q.Liu, T.Liu, S.Hayakawa, L.Yang, H.Shimizu, C.B.Hamill, A.St J.Murphy, J.Su, X.Fang, K.Y.Chae, M.S.Kwag, S.M.Cha, N.N.Duy, N.K.Uyen, D.H.Kim, R.G.Pizzone, M.La Cognata, S.Cherubini, S.Romano, A.Tumino, J.Liang, A.Psaltis, M.Sferrazza, D.Kim, Y.Y.Li, S.Kubono Advancement of Photospheric Radius Expansion and Clocked Type-I X-Ray Burst Models with the New 22Mg(α, p)25Al Reaction Rate Determined at the Gamow Energy NUCLEAR REACTIONS 1H(25Al, p), (25Al, p'), (25Al, X), E=142 MeV; measured reaction products, Ep, Ip, Eγ, Iγ. 26Si; deduced σ(θ), level energies, J, π, resonance parameters, astrophysical reaction rates. Comparison with available data.
doi: 10.1103/physrevlett.127.172701
2021LI61 Phys.Rev. C 104, 054302 (2021) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, X.G.Cao, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, J.C.Wang, D.X.Wang, S.Y.Zhang, Y.D.Liu, X.Ma, C.W.Ma, Y.T.Wang, Z.D.An, J.J.He, J.Su, L.Y.Zhang, Y.X.Yang, W.B.Liu, W.Q.Su New experimental measurement of natEr(n, γ) cross sections between 1 and 100 eV NUCLEAR REACTIONS 162,164,166,167,168,170Er, 12,13C, 197Au(n, γ), E=0.001-100 keV; measured E(n), I(n), Eγ, Iγ using C6D6 liquid scintillator and a silicon monitor and natural Er, C and Au targets at the China spallation neutron source (CSNS) facility; deduced neutron-capture σ(E), capture yields as function of E(n), neutron resonances in Er isotopes in the 1-100 eV region. 162,164,166,167,168Er; deduced energies of 43 neutron resonances (nine for 162Er, five for 164Er, three for 166Er, 25 for 167Er, one for 168Er), cross sections, widths Γγ and Γn by R-matrix analysis. Comparison with previous experimental data, and with data in evaluated databases ENDF/B-VIII.0, ENDF/B-VII.1, JENDL-4.0, and ROSFOND-2010.
doi: 10.1103/PhysRevC.104.054302
2021MA60 Prog.Part.Nucl.Phys. 121, 103911 (2021) C.-W.Ma, H.-L.Wei, X.-Q.Liu, J.Su, H.Zheng, W.P.Lin, Y.-X.Zhang Nuclear fragments in projectile fragmentation reactions
doi: 10.1016/j.ppnp.2021.103911
2021ME13 Chin.Phys.C 45, 054001 (2021) B.Mei, D.L.Balabanski, W.Hua, Y.-H.Zhang, X.-H.Zhou, C.-X.Yuan, J.Su Fusion reactions around the barrier for Be+238U NUCLEAR REACTIONS 238U(9Be, 5n)242Cm, E=35-70 MeV; measured reaction products, Eα, Iα; deduced σ. Comparison with model calculations through two different codes, namely HIVAP2 and KEWPIE2, using two methods (i.e., WKB and EBD) for the capture probability.
doi: 10.1088/1674-1137/abe36c
2021SO19 Chin.Phys.C 45, 044101 (2021) Nucleon stripping in deuteron-induced spallation reactions at hundreds MeV/nucleon NUCLEAR REACTIONS 208Pb(n, X), (p, X), E=200 MeV/nucleon; 12C, 27Al, 65Cu, 120Sn, 208Pb(d, X), E<1000 MeV; analyzed available data; calculated σ.
doi: 10.1088/1674-1137/abde31
2021SU11 Appl.Radiat.Isot. 174, 109752 (2021) Production of high-energy neutrons by interaction of a deuteron beam with matter NUCLEAR REACTIONS 12C, 208Pb(p, n), E=256 MeV; 12C(d, n), E=100 MeV; analyzed available data; calculated neutron products σ(θ, E) by the IQMD model.
doi: 10.1016/j.apradiso.2021.109752
2021WA41 Phys.Rev. C 104, 034317 (2021) Providing physics guidance in Bayesian neural networks from the input layer: The case of giant dipole resonance predictions NUCLEAR STRUCTURE A=16-240; 124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160Nd; analyzed giant-dipole resonance (GDR) data using Bayesian neural network (BNN) approach; evaluated and predicted nuclear data. Pearson's correlation coefficients applied for statistical dependence between nuclear properties in the ground state and the GDR energies. Relevance to discovering physics effects from complex nuclear data.
doi: 10.1103/PhysRevC.104.034317
2021WA55 Chin.Phys.C 45, 124103 (2021) Modeling complex networks of nuclear reaction data for probing their discovery processes NUCLEAR REACTIONS 63Cu(n, 2n), 6Li(γ, xn), E not given; analyzed available data; deduced model to build networks for discovery processes of nuclear reaction data based on a Bayesian statistics-based approach.
doi: 10.1088/1674-1137/ac23d5
2021ZH46 Chin.Phys.C 48, 084108 (2021) H.Zhang, Z.i-H.Li, J.Su, Y.-J.Li, C.Chen, L.Zhang, F.-Q.Cao, Y.-P.Shen, W.Nan, W.-K.Nan, X.-Y.Li, L.-H.Chen, G.Lian, B.-Q.Cui, B.Guo, W.-P.Liu Direct measurement of the resonance strengths and branching ratios of low-energy (p, γ) reactions on Mg isotopes NUCLEAR REACTIONS 24,25,26Mg(p, γ), E=220-400 keV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, yields, resonances, branching ratios, resonance strengths. JUNA experiment, comparison with NACRE data.
doi: 10.1088/1674-1137/ac06aa
2021ZH53 Phys.Rev.Lett. 127, 152702 (2021) L.Y.Zhang, J.Su, J.J.He, M.Wiescher, R.J.deBoer, D.Kahl, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, X.D.Tang, H.W.Zhao, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, B.Guo, S.W.Xu, J.Y.Li, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, X.H.Zhou, Y.H.Zhang, F.S.Zhang, Z.G.Hu, H.S.Xu, J.P.Chen, W.P.Liu Direct Measurement of the Astrophysical 19F(p, αγ)16O Reaction in the Deepest Operational Underground Laboratory NUCLEAR REACTIONS 19F(p, α), E(cm)=72.4-188.8 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factors, reaction rates. The China Jinping Underground Laboratory (CJPL), JUNA accelerator.
doi: 10.1103/physrevlett.127.152702
2021ZH58 Phys.Rev. C 104, 044606 (2021) Unified description of fusion and multinucleon transfer processes within the dinuclear system model NUCLEAR REACTIONS 238U(48Ca, X), (48Ca, 3n), (48Ca, 4n), E(cm)=182-204 MeV; calculated potential energy surface (PES) as a function of mass asymmetry and β2, capture σ(E), fusion probability as function of incident energy and deformation parameter β2, and evaporation residue (ER) σ(E) using DNS-SYSU code. 243Am(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=25-48 MeV; 244Pu, 248Cm(48Ca, 3n), (48Ca, 4n), E*=30-58 MeV; 249Cf(48Ca, 3n), E*=28-42 MeV; calculated evaporation residue σ(E). 238U(48Ca, X), E(cm)=180, 196, 204 MeV; calculated mass distribution of primary fragments, total kinetic energy (TKE)-mass distributions of multi-nucleon transfer (MNT) products. 238U(48Ca, F), E(cm)=196 MeV; calculated Production cross sections of Ac (A=220-236), Th (A=223-238), Pa (A=227-240), U (A=229-242), and Np (A=232-240). 238U(48Ca, X)60Ca/200W/245U/246Np/281Cn/282Cn/283Cn/284Cn/285Cn, E(cm)=180-270 MeV; calculated production σ(E). Dinuclear system (DNS) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.044606
2020GA03 Phys.Rev. C 101, 014612 (2020) L.Gan, H.B.Sun, Z.H.Li, S.P.Hu, Y.J.Li, J.Su, B.Guo, S.Q.Yan, Y.B.Wang, S.Zeng, Z.Y.Han, X.Y.Li, D.H.Li, T.L.Ma, Y.P.Shen, Y.Su, E.T.Li, W.P.Liu Experimental study of the spectroscopic factors of 116-125Sn NUCLEAR REACTIONS 116,118,120,122,124Sn(p, d), E=18.0 MeV; 116,118,120,122,124Sn(d, p), E=12.0 MeV; measured E(p), I(p), E(d), I(d), σ(θ) using the high-precision Q3D magnetic spectrograph at the CIAE-Beijing HI-13 tandem accelerator. 115,117,119,121,123,125Sn; deduced levels, L-transfers, J, π, spectroscopic factors (SFs). DWBA analysis of σ(θ) data and extraction of the neutron spectroscopic factors using two different sets of systematic optical potential parameters. Comparison with previous experimental data. Proposed a linear formula to relate SFs with S(n).
doi: 10.1103/PhysRevC.101.014612
2020LI31 Phys.Rev. C 102, 025804 (2020) Y.J.Li, Z.H.Li, E.T.Li, X.Y.Li, T.L.Ma, Y.P.Shen, J.C.Liu, L.Gan, Y.Su, L.H.Qiao, Z.Y.Han, Y.Zhou, J.Su, S.Q.Yan, S.Zeng, Y.B.Wang, B.Guo, G.Lian, D.Nan, X.X.Bai, W.P.Liu Indirect measurement of the 57.7 keV resonance strength for the astrophysical γ-ray source of the 25Mg(p, γ)26Al reaction NUCLEAR REACTIONS 24,25Mg(7Li, 6He), (7Li, 7Li), E=31.5 MeV; measured 6He and 7Li particle spectra using ΔE-E telescope of Si detectors, σ(θ) using Q3D magnetic spectrometer at the HI-13 tandem accelerator of CIAE-Beijing. 26Al; deduced levels, J, π, spectroscopic factors. DWBA analysis of σ(θ) data using the code FRESCO, with Woods-Saxon potential parameters deduced from analysis of the present data and the literature data for 27Al(6Li, 6Li) reaction. 25Mg(p, γ)26Al; deduced Γp and resonance strength of 57.7-keV proton resonance in 26Al. 25Mg(p, γ)26Al, T9=0.1-10; calculated astrophysical reaction rates for the ground and isomeric states in 26Al, and compared with the results in the NACRE database.
doi: 10.1103/PhysRevC.102.025804
2020RO16 Chin.Phys.C 44, 104003 (2020) C.-H.Rong, G.-L.Zhang, L.Gan, Z.-Ho.Li, L.C.Brandao, E.N.Cardozo, M.R.Cortes, Y.-J.Li, Ju.Su, S.-Q.Yan, S.Zeng, G.Lian, B.Guo, Y.-B.Wang, W.-P.Liu, J.Lubian The angular distributions of elastic scattering of 12, 13C+Zr NUCLEAR REACTIONS 90,91,92,94,96Zr(12C, 12C), (13C, 13C), E=66, 64 MeV; measured reaction products; deduced σ, the neutron spectroscopic amplitudes using the optical model and coupled channel calculations.
doi: 10.1088/1674-1137/abab8d
2020SH09 Phys.Rev.Lett. 124, 162701 (2020) Y.P.Shen, B.Guo, R.J.deBoer, Z.H.Li, Y.J.Li, X.D.Tang, D.Y.Pang, S.Adhikari, C.Basu, J.Su, S.Q.Yan, Q.W.Fan, J.C.Liu, C.Chen, Z.Y.Han, X.Y.Li, G.Lian, T.L.Ma, W.Nan, W.K.Nan, Y.B.Wang, S.Zeng, H.Zhang, W.P.Liu Constraining the External Capture to the 16O ground State and the E2 S Factor of the 12C(α, γ)16O reaction NUCLEAR REACTIONS 12C(11B, 7Li)16O, E=50 MeV; measured reaction products; deduced σ(θ), the ground state asymptotic normalization coefficients, S-factors. Comparison with available data.
doi: 10.1103/PhysRevLett.124.162701
2020SU12 Phys.Rev. C 101, 044606 (2020) Constraints on the effective mass splitting by the isoscalar giant quadrupole resonance NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated correlation between the square of the excitation energies of isoscalar giant quadrupole resonances (ISGQRs) and the reciprocal of the weighted effective masses using the microscopic Langevin equation with particle density and kinetic-energy density from the Thomas-Fermi (TF) approach and the Hartree-Fock-Bogolyubov (SHFB) model. Comparison with experimental data. A=30-240; compiled experimental excitation energies of the ISGQRs as a function of mass number, and compared with several theoretical calculations.
doi: 10.1103/PhysRevC.101.044606
2020SU18 Chin.Phys.C 44, 084106 (2020) J.Su, L.Zhu, C.Guo, F.-S.Zhang Isospin dependence of projectile fragmentation at hundreds of MeV/u NUCLEAR REACTIONS 120Sn(124Sn, X), (107Sn, X), E=600 MeV/nucleon; 208Pb(136Xe, X), (124Xe, X), E=1000 MeV/nucleon; analyzed available data; deduced isospin observables, neutron-to-proton ratios of the light particles emitted from the fragmenting. Isospin-dependent quantum molecular dynamics (IQMD) model and permitting only evaporation in the statistical model GEMINI, the IQMD+GEMINI model.
doi: 10.1088/1674-1137/44/8/084106
2020XU02 Phys.Rev. C 101, 024609 (2020) Probing the deuteron breakup and linking the cross sections of residue production between the neutron- and deuteron-induced spallation at 500 MeV/nucleon NUCLEAR REACTIONS 56Fe, 115In(p, X), E=800, 1500 MeV/nucleon; 137Cs(d, X), E=500 MeV/nucleon; calculated double-differential σ(θ, E) for neutron production, correlation of longitudinal momenta between neutron and proton from the deuteron, contributions of deuteron absorbing, neutron stripping, proton stripping, and elastic breakup of deuteron to the energy distribution of neutrons. 2H(137Cs, X), E=500 MeV/nucleon; calculated transverse momentum vs longitudinal momentum of neutrons and proton in d+137Cs spallation. 1,2H(136Xe, X), E=500 MeV/nucleon; calculated isotopic production cross sections of residual nuclei with Z=41-56 and N-Z=8-30. 1n, 2H(137Cs, X), E=500 MeV/nucleon; calculated isotopic production cross sections of residual nuclei with Z=33-56 and N-Z=4-30. Isospin-dependent quantum molecular dynamics (IQMD) model for the spallation process, and statistical model GEMINI based on the Hauser-Feshbach formalism to describe the deexcitation of the hot fragments. Comparison with available experimental data.
doi: 10.1103/PhysRevC.101.024609
2020ZH22 Int.J.Mod.Phys. E29, 2030004 (2020) L.Zhu, C.Li, C.-C.Guo, J.Su, P.W.Wen, G.Zhang, F.-S.Zhang Theoretical progress on production of isotopes in the multinucleon transfer process NUCLEAR REACTIONS 238U(64Ni, X), E(cm)=307.5 MeV; 208Pb(124Xe, X), E(cm)=50 MeV; 186W(160Gd, X), E=503 MeV; calculated transfer σ for production of neutron-rich transuranium nuclei.
doi: 10.1142/S0218301320300040
2019MA31 Nucl.Phys. A986, 26 (2019) T.L.Ma, B.Guo, Z.H.Li, Y.J.Li, D.Y.Pang, Y.L.Han, Y.P.Shen, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu Precision measurement of the angular distribution for the 16O(d, p)17O transfer reaction to the ground state of 17O NUCLEAR REACTIONS 16O(d, p)17O, E=15 MeV; measured Ep, Ip(θ); deduced σ(θ) for reactions to 17O gs, spectroscopic factors, ANC; calculated σ(θ) for reactions to 17O gs using DWBA, ADWA (Adiabatic DWBA) and Continuum Discretized Coupled Channel (CDCC) vs radius parameter of Woods-Saxon potential with the same optical potential parameters in ADWA and CDCC. SF and ANC for 17O compared with published results in heavy ion transfer and with shell model calculations.
doi: 10.1016/j.nuclphysa.2019.03.004
2019ON02 Phys.Rev. C 100, 044617 (2019) A.Ono, J.Xu, M.Colonna, P.Danielewicz, C.M.Ko, M.B.Tsang, Y.-J.Wang, H.Wolter, Y.-X.Zhang, L.-W.Chen, D.Cozma, H.Elfner, Z.-Q.Feng, N.Ikeno, B.-A.Li, S.Mallik, Y.Nara, T.Ogawa, A.Ohnishi, D.Oliinychenko, J.Su, T.Song, F.-S.Zhang, Z.Zhang Comparison of heavy-ion transport simulations: Collision integral with pions and Δ resonances in a box
doi: 10.1103/PhysRevC.100.044617
2019SH11 Phys.Rev. C 99, 025805 (2019) Y.P.Shen, B.Guo, Z.H.Li, Y.J.Li, D.Y.Pang, S.Adhikari, Z.D.An, J.Su, S.Q.Yan, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, D.H.Li, E.T.Li, X.Y.Li, G.Lian, J.C.Liu, T.L.Ma, C.J.Pei, Y.Su, Y.B.Wang, S.Zeng, Y.Zhou, W.P.Liu Astrophysical SE2 factor of the 12C (α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; 16O(7Li, 7Li), E=26 MeV; measured charged-particle spectra, differential σ(θ) using the Q3D magnetic spectrograph at the HI-13 tandem accelerator of the CIAE-Beijing. 12C(α, γ), E(cm)<5 MeV; deduced astrophysical SE2(300) factor of the ground state. 16O; deduced asymptotic normalization coefficient (ANC) and reduced α width of the 6.917-MeV level from finite-range distorted wave Born approximation (FRDWBA) and coupled-reaction-channel (CRC) analysis using FRESCO code. Comparison with previous experimental values, and with theoretical model predictions. R-matrix analysis of scattering data.
doi: 10.1103/PhysRevC.99.025805
2019SH37 Phys.Lett. B 797, 134820 (2019) Y.P.Shen, B.Guo, T.L.Ma, D.Y.Pang, D.D.Ni, Z.Z.Ren, Y.J.Li, Z.D.An, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, Z.H.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu First experimental constraint of the spectroscopic amplitudes for the α-cluster in the 11B ground state NUCLEAR REACTIONS 7Li(6Li, d), E=24 MeV; measured reaction products; deduced spectroscopic amplitudes (SA) for the α-cluster in the 11B ground state. Comparison with available data.
doi: 10.1016/j.physletb.2019.134820
2019SU08 Chin.Phys.C 43, 064109 (2019) Constraining symmetry energy at subnormal density by isovector giant dipole resonances of spherical nuclei NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated energy per nucleon as a function of the collective variable X in the isovector giant dipole resonance (IVGDR), density distribution of the static Hartree-Fock ground state. Comparison with experimental data.
doi: 10.1088/1674-1137/43/6/064109
2019SU17 Phys.Rev. C 100, 014602 (2019) Uniform description of breakup mechanisms in central collision, projectile fragmentation, and proton-induced spallation NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; 63Cu(197Au, X), E=600 MeV/nucleon; 12C(197Au, X), E=1000 MeV/nucleon; 1H(56Fe, X), E=1000 MeV/nucleon; calculated charge distribution of fragments, multiplicity of intermediate mass fragments with Z=3-30, first and second fragment asymmetries versus the analogous bound charge. 48Ti(48Ti, X), E=30 MeV/nucleon; 120Sn(120Sn, X), E=600 MeV/nucleon; 1H(90Zr, X), E=2000 MeV/nucleon; calculated energy-density trajectories of the projectile centers, and fragment mass-excitation, correlations between the intermediate mass fragment (IMF) multiplicity and the total bound charge of the productions in the central collision, projectile fragmentation, and proton-induced spallation. Isospin-dependent quantum molecular dynamics (IQMD) model for breakup mechanisms in central collision, with the evaporations of light particles from the prefragments described by the statistical code GEMINI. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.014602
2019WE10 Chin.Phys.C 43, 074103 (2019) H.-L.Wei, Y.-D.Song, C.-W.Ma, Z.-H.Li, J.Su Cross-section prediction for isotopes near neutron drip line in 70, 80Zn projectile fragmentation reactions NUCLEAR REACTIONS 9Be(70Zn, X)59Ca/60Ca, E=345 MeV/nucleon; analyzed available data. 66,70Ca; deduced parameters, σ for production of very neutron rich calcium nuclei.
doi: 10.1088/1674-1137/43/7/074103
2019YA14 Chin.Phys.C 43, 104101 (2019) Prediction of the cross-sections of isotopes produced in deuteron-induced spallation of long-lived fission products NUCLEAR REACTIONS 90Sr, 93Zr, 107Pd, 137Cs(d, X), E=200, 500, 1000 MeV/nucleon; calculated σ. Comparison with available data.
doi: 10.1088/1674-1137/43/10/104101
2019ZH12 Chin.Phys.C 43, 024103 (2019) A dynamical description of the 136Xe + p spallation at 1000 MeV/nucleon NUCLEAR REACTIONS 136Xe(p, X), E=1000 MeV/nucleon; calculated σ, mean neutron-to-proton ratio. Comparison with available data.
doi: 10.1088/1674-1137/43/2/024103
2019ZH13 Phys.Lett. B 791, 20 (2019) L.Zhu, C.Li, J.Su, C.-C.Guo, W.Hua Advantages of the multinucleon transfer reactions based on 238U target for producing neutron-rich isotopes around N=126 NUCLEAR REACTIONS 238U(186W, X), (160Gd, X), E(cm)=660, 475 MeV; analyzed available data; deduced mechanism of multinucleon transfer (MNT) reactions for producing neutron-rich heavy nuclei around N=126 using dinuclear system (DNS) model and isospin-dependent quantum molecular dynamics (IQMD) model.
doi: 10.1016/j.physletb.2019.02.015
2019ZH37 Phys.Rev. C 100, 024603 (2019) F.Zhang, C.Li, P.-W.Wen, J.-W.Liu, J.Su, F.-S.Zhang Time dependence of the thermal-photon thermometer NUCLEAR REACTIONS 190W, 197Au(36Ar, X), E=60 MeV/nucleon; 168Er(36Ar, X), E=30 MeV/nucleon; 171Yb(36Ar, X), E=35, 40 MeV/nucleon; 176Lu(36Ar, X), E=40 MeV/nucleon; 188Os(36Ar, X), E=55, 60, 65 MeV/nucleon; 206Bi, 206Rn, 204Hg(36Ar, X), E=95 MeV/nucleon; calculated the time dependence of density contours, photon production rates, temperatures, mass, N/Z ratio, quadrupole moment. Systematic study of the thermal-photon thermometer via the isospin-dependent quantum molecular dynamics (IQMD) model.
doi: 10.1103/PhysRevC.100.024603
2018GA19 Phys.Rev. C 97, 064614 (2018) L.Gan, H.B.Sun, Z.H.Li, Y.J.Li, J.Su, B.Guo, S.Q.Yan, Y.B.Wang, S.Zeng, Z.Y.Han, X.Y.Li, D.H.Li, T.L.Ma, Y.P.Shen, Y.Su, E.T.Li, S.P.Hu, W.P.Liu Experimental study of the spectroscopic factors of 90-97Zr NUCLEAR REACTIONS 90,92,94,96Zr(12C, 12C), (12C, 13C), E=66 MeV; 90,92,94,96Zr(13C, 13C), (13C, 12C), E=64 MeV; measured particle spectra, differential σ(θ) using Q3D magnetic spectrograph at the HI-13 tandem accelerator facility of the CIAE, Beijing; deduced neutron spectroscopic factors using distorted-wave Born approximation (DWBA) calculations. Comparison of spectroscopic results with previous experiments. Relevance to neutron capture reactions in s process for synthesis of heavy elements.
doi: 10.1103/PhysRevC.97.064614
2018LI18 Chin.Phys.C 42, 044001 (2018) E.-T.Li, Z.H.Li, S.-Q.Yan, J.Su, B.Guo, Y.-J.Li, Y.-B.Wang, G.Lian, S.Zeng, S.-Z.Chen, S.-B.Ma, X.-Q.Li, C.He, H.-B.Sun, W.-P.Liu Measurement of the 2H(7Be, 6Li)3He reaction rate and its contribution to the primordial lithium abundance NUCLEAR REACTIONS 2H(7Be, 6Li)3He, E=17.7, 30.2 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ, reaction rates. Comparison with theoretical calculations.
doi: 10.1088/1674-1137/42/4/044001
2018LI24 Chin.Phys.C 42, 065001 (2018) Z.-H.Li, E.-T.Li, J.Su, Y.-J.Li, Y.-B.Wang, S.-Q.Yan, B.Guo, D.Nan, W.-P.Liu New determination of the 7Be ground state spectroscopic factor and the 6Li(p, γ)7Be astrophysical S(E)factors NUCLEAR REACTIONS 7Be(d, 3He)6Li, E(cm)=6.7 MeV; measured reaction products; deduced σ(θ). 6Li(p, γ)7Be, E(cm)<1 MeV; analyzed available data; deduced S factors. Comparison with DWBA calculation code TWOFNR.
doi: 10.1088/1674-1137/42/6/065001
2018LI33 Phys.Rev. C 98, 014618 (2018) F.Li, L.Zhu, Z.-H.Wu, X.-B.Yu, J.Su, C.-C.Guo Predictions for the synthesis of superheavy elements Z=119 and 120 NUCLEAR REACTIONS 238U, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; calculated evaporation residue σ(E), and compared with available experimental data. 252Es(40Ca, 3n), E(cm)=204.08 MeV; 252Es(42Ca, 3n), E(cm)=203.00 MeV; 249Cf(45Sc, 3n), E(cm)=211.09 MeV; 255Es(40Ca, 4n), E(cm)=207.02 MeV; 254Es(40Ca, 3n), E(cm)=203.60 MeV; 247Bk(47Ti, 3n), E(cm)=219.19 MeV; 248Bk(46Ti, 3n), E(cm)=217.76 MeV; 242Cm(51V, 2n), E(cm)=225.86 MeV; 248Cf(45Sc, 2n), E(cm)=209.29 MeV; 241Am(52Cr, 2n), E(cm)=231.94 MeV; 252Es(44Ca, 3n), E(cm)=204.27 MeV; 253Es(43Ca, 3n), E(cm)=202.49 MeV; 254Es(42Ca, 3n), E(cm)=201.65 MeV; 251Cf(45Sc, 3n), E(cm)=210.03 MeV; 249Bk(47Ti, 3n), E(cm)=217.18 MeV; 248Bk(48Ti, 3n), E(cm)=219.47 MeV; 245Cm(51V, 3n), E(cm)=229.29 MeV; 247Bk(49Ti, 3n), E(cm)=222.17 MeV; 246Cm(50V, 3n), E(cm)=225.70 MeV; 244Cm(51V, 2n), E(cm)=224.00 MeV; 255Es(42Ca, 4n), E(cm)=205.95 MeV; 243Am(53Cr, 3n), E(cm)=236.20 MeV; 254Es(43Ca, 4n), E(cm)=206.90 MeV; 253Es(44Ca, 4n), E(cm)=210.94 MeV; 243Am(52Cr, 2n), E(cm)=229.49 MeV; 254Es(44Ca, 3n), E(cm)=201.64 MeV; 255Es(43Ca, 3n), E(cm)=201.49 MeV; 255Es(44Ca, 4n), E(cm)=207.59 MeV; 252Es(46Ca, 3n), E(cm)=206.00 MeV; 248Bk(50Ti, 3n), E(cm)=222.48 MeV; 247Cm(51V, 3n), E(cm)=226.83 MeV; 254Cf(45Sc, 4n), E(cm)=211.93 MeV; 249Bk(49Ti, 3n), E(cm)=218.88 MeV; 254Es(46Ca, 3n), E(cm)=203.64 MeV; 255Es(46Ca, 4n), E(cm)=210.13 MeV; 252Es(48Ca, 3n), E(cm)=208.42 MeV; 255Es(46Ca, 3n), E(cm)=204.13; 254Es(48Ca, 3n), E(cm)=205.96 MeV; 255Es(48Ca, 4n), E(cm)=212.72 MeV; 242Cm(50Cr, 2n), E(cm)=234.22 MeV; 249Cf(46Ti, 3n), E(cm)=222.89 MeV; 248Cf(46Ti, 2n), E(cm)=219.12 MeV; 257Fm(40Ca, 5n), E(cm)=222.66 MeV; 257Fm(40Ca, 4n), E(cm)=211.66 MeV; 257Fm(40Ca, 3n), E(cm)=205.66 MeV; 251Cf(46Ti, 3n), E(cm)=220.39 MeV; 252Es(45Sc, 3n), E(cm)=214.17 MeV; 250Cf(46Sc, 2n), E(cm)=218.88 MeV; 247Bk(50V, 3n), E(cm)=231.13 MeV; 244Cm(52Cr, 2n), E(cm)=234.88 MeV; 245Cm(52Cr, 3n), E(cm)=240.80 MeV; 243Cm(53Cr, 2n), E(cm)=236.02 MeV; 247Cm(50Cr, 3n), E(cm)=235.12 MeV; 257Fm(42Ca, 3n), E(cm)=205.29 MeV; 254Es(45Sc, 3n), E(cm)=213.40 MeV; 257Fm(43Ca, 4n), E(cm)=210.97 MeV; 257Fm(44Ca, 3n), E(cm)=205.27 MeV; 257Fm(46Ca, 3n), E(cm)=207.84 MeV; 250Cm(53Cr, 3n), E(cm)=234.59 MeV; 257Fm(48Ca, 3n), E(cm)=211.07 MeV; calculated production σ for Z=119 and 120 superheavy isotopes. Dinuclear system (DNS) model.
doi: 10.1103/PhysRevC.98.014618
2018SU08 Phys.Rev. C 97, 054604 (2018) Influence of the nuclear level density on the odd-even staggering in 56Fe + spallation at energies from 300 to 1500 MeV/nucleon NUCLEAR REACTIONS 1H(56Fe, X), E=300-1500 MeV/nucleon; calculated level-density parameter, energy backshift, σ(E), differential σ(E), odd-even staggering (OES), and neutron- and proton-separation energies for Z=8-26, Tz=-1/2, 0, +1/2, +1 residual nuclei; deduced influence of level density on OES. 54Fe, 52Mn; calculated level densities as function of excitation energy. Calculations performed using isospin-dependent quantum molecular dynamics (IQMD) model using statistical model GEMINI code. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.054604
2018SU12 Phys.Rev. C 98, 014610 (2018) J.Su, W.Trautmann, L.Zhu, W.-J.Xie, F.-S.Zhang Dynamical properties and secondary decay effects of projectile fragmentations in 124Sn, 107Sn + 120Sn collisions at 600 MeV/nucleon NUCLEAR REACTIONS 120Sn(124Sn, X), (107Sn, X), E=600 MeV/nucleon; calculated mass number and excitation energy of fragments, longitudinal momenta, mean multiplicity of intermediate mass fragments (IMFs), σ(Z) of fragments, mean neutron-to-proton ratios of light fragments. Isospin-dependent quantum molecular dynamics model (IQMD) with and without the GEMINI statistical code. Comparison with experimental data for fragment yields from ALADIN Collaboration.
doi: 10.1103/PhysRevC.98.014610
2018SU17 Phys.Rev. C 98, 024315 (2018) Isoscalar giant monopole resonance within the Bohr-Mottelson model NUCLEAR STRUCTURE A=20-240; analyzed excitation energies and incompressibility parameters, widths, surface and symmetry parameters, Coulomb parameter of the incompressibility of the Isoscalar giant monopole resonance (ISGMR) as a function of the mass number in nuclei from 12C to 238U using Bohr-Mottelson model. Comparison with other theoretical predictions.
doi: 10.1103/PhysRevC.98.024315
2018WA34 Yuan.Wul.Ping. 35, 445 (2018); Nucl.Phys.Rev. 35, 445 (2018) Y.Wang, J.Su, Z.Han, B.Tang, B.Cui, T.Ge, Y.Lu, Z.Chen, B.Guo, X.Li, Y.Li, Z.Li, G.Lian, T.Ma, Y.Ma, Y.Shen, Y.Su, C.Wang, H.Wu, S.Yan, S.Zeng, Y.Zheng, C.Zhou, Y.Dang, G.Fu, Y.He, F.Liu, D.Wu, T.Zhang, W.Liu, for the BRIF collaboration Study of the Exotic Decay Mode of 20Na with an Intense ISOL Beam RADIOACTIVITY 20Na(β+α) [from 24Mg(p, nα), E<100 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced γ-ray energies and intensities, exotic β-γ-α decay mode.
doi: 10.11804/NuclPhysRev.35.04.445
2018WU06 Phys.Rev. C 97, 064609 (2018) Z.-H.Wu, L.Zhu, F.Li, X.-B.Yu, J.Su, C.-C.Guo Synthesis of neutron-rich superheavy nuclei with radioactive beams within the dinuclear system model NUCLEAR REACTIONS 242,244Pu, 243Am, 245,248,250Cm, 249Bk, 250,251Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; 234Th(42S, 2n), (42S, 3n), (42S, 4n), (42S, 5n), E*=20-65 MeV; 234Th, 244Pu(46Ar, 2n), (46Ar, 3n), (46Ar, 4n), (46Ar, 5n), E*=20-65 MeV; 234Th, 238U, 248Cm, 255Es(44Cl, 2n), (44Cl, 3n), (44Cl, 4n), (44Cl, 5n), E*=20-65 MeV; 228Ra(45Cl, 2n), (45Cl, 3n), (45Cl, 4n), (45Cl, 5n), E*=20-65 MeV; 244Pu, 248Cm(43Cl, 2n), (43Cl, 3n), (43Cl, 4n), (43Cl, 5n), E*=20-65 MeV; 244Pu, 254Cf, 255Es(41S, 2n), (41S, 3n), (41S, 4n), (41S, 5n), E*=20-65 MeV; 257Fm(42Ar, 2n), (42Ar, 3n), (42Ar, 4n), (42Ar, 5n), E*=20-65 MeV; 260Md(38Cl, 2n), (38Cl, 3n), (38Cl, 4n), (38Cl, 5n), E*=20-65 MeV; calculated evaporation residue σ. 228Ra(45Cl, 2n), E*=36.0 MeV; 228Ra(46Cl, 3n), E*=46.0 MeV; 226Ra(47Cl, 2n), E*=36.0 MeV; 234Th(42S, 4n), E*=43.0 MeV; 228Ra(46Ar, 2n), E*=34.0 MeV; 234Th(43S, 5n), E*=51.0 MeV; 234Th(42S, 3n), E*=41.0 MeV; 234Th(43S, 4n), E*=46.0 MeV; 234Th(44S, 5n), E*=59.0 MeV; 234Th(44Cl, 2n), E*=37.0 MeV; 234Th(45Cl, 3n), E*=44.0 MeV; 228Ra(50K, 2n), E*=36.0 MeV; 234Th(46Ar, 2n), E*=34.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 238U(42S, 2n), E*=37.0 MeV; 238U(44Cl, 3n), E*=38.0 MeV; 238U(43Cl, 2n), E*=36.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 234Th(47K, 2n), E*=33.0 MeV; 244Pu(41S, 3n), E*=38.0 MeV; 244Pu(42S, 4n), E*=42.0 MeV; 238U(46Ar, 2n), E*=33.0 MeV; 244Pu(43Cl, 4n), E*=44.0 MeV; 242Pu(44Cl, 3n), E*=37.0 MeV; 244Pu(42Cl, 3n), E*=38.0 MeV; 244Pu(46Ar, 4n), E*=38.0 MeV; 244Pu(45Ar, 3n), E*=44.0 MeV; 242Pu(46Ar, 2n), E*=33.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 4n), E*=39.0 MeV; 250Cm(43Cl, 5n), E*=45.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 253Cf(42S, 5n), E*=40.0 MeV; 250Cm(44Ar, 4n), E*=37.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 254Cf(42Cl, 5n), E*=40.0 MeV; 253Cf(43Cl, 5n), E*=39.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 253Cf(43Cl, 4n), E*=36.0 MeV; 254Cf(42Cl, 4n), E*=37.0 MeV; 250Cm(48Ca, 4n), E*=35.0 MeV; 248Cm(48Ca, 2n), E*=31.0 MeV; 250Cm(46Ca, 2n), E*=35.0 MeV; 255Es(44Cl, 5n), E*=40.0 MeV; 254Cf(44Ar, 4n), E*=36.0 MeV; 257Fm(41S, 4n), E*=37.0 MeV; 250Cm(48Ca, 3n), E*=31.0 MeV; 255Es(44Cl, 4n), E*=36.0 MeV; 253Cf(46Ar, 4n), E*=34.0 MeV; 254Cf(46Ar, 5n), E*=41.0 MeV; 250Cf(48Ca, 3n), E*=34.0 MeV; 250Cm(49Ti, 4n), E*=42.0 MeV; 252Cf(46Ca, 3n), E*=36.0 MeV; 260Md(38Cl, 3n), E*=41.0 MeV; 260Md(39Cl, 4n), E*=42.0 MeV; 257Fm(42Ar, 4n), E*=41.0 MeV; 251Cf(48Ca, 3n), E*=30.0 MeV; 252Cf(48Ca, 4n), E*=38.0 MeV; 250Cm(49Ti, 3n), E*=34.0 MeV; 257Fm(42Ar, 3n), E*=33.0 MeV; 257Fm(43Ar, 4n), E*=38.0 MeV; 260Md(39Cl, 3n), E*=37.0 MeV; 244Pu(43Cl, n), E*=40.0 MeV; 238Cm(48Ca, 2np), E*=41.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 248Cm(48Ca, 2nα), E*=46.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, 2np), E*=35.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, np), E*=40.0 MeV; 244Pu(48Ca, 3np), E*=45.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 245Cm(48Ca, np), E*=32.0 MeV; 249Bk(48Ca, 2nα), E*=37.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 248Cm(48Ca, 3np), E*=44.0 MeV; 249Bk(48Ca, nα), E*=32.0 MeV; calculated evaporation residue σ, and optimal incident beam energies. 48Ca(238U, 2n), (238U, 3n), (238U, 4n), E(cm)=184.13-214.13 MeV; calculated evaporation residue σ, potential energy surface, driving potential, survival and complete fusion probabilities, and capture σ. Dinuclear system model. 271Db, 272,273Sg, 276Bh, 278Hs, 279Mt, 282Ds, 283Rg, 286Cn, 287,288Nh, 290Fl, 291,292Mc, 294,295Lv, 295,296Og; calculated evaporation residue σ, and optimal incident beam energies for various reactions. Comparison with available experimental data. Relevance to synthesis of neutron-rich superheavy nuclei using radioactive ion beams, such as those at ATLAS-ANL.
doi: 10.1103/PhysRevC.97.064609
2018XI05 Phys.Rev. C 97, 064608 (2018) W.-J.Xie, J.Su, L.Zhu, F.-S.Zhang Effects of the pion-nucleon potential in 197Au + 197Au collisions at 1.5 GeV/nucleon NUCLEAR REACTIONS 197Au(197Au, X), E=1.5 GeV/nucleon; calculated pion multiplicity, excitation function of pion multiplicity, rapidity distributions of directed and elliptic flows, rapidity dependence of the and centrality dependence of midrapidity and elliptic flows, polar angle distributions of π+ and π-, transverse momentum dependence of the strength function of the azimuthal anisotropy, using isospin-dependent quantum molecular dynamics (IQMD) model using various sets of the pion-nucleon (πN) potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.064608
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
2018ZH17 Phys.Rev. C 97, 044614 (2018) L.Zhu, P.-W.Wen, C.-J.Lin, X.-J.Bao, J.Su, C.Li, C.-C.Guo Shell effects in a multinucleon transfer process NUCLEAR REACTIONS 198Pt(136Xe, X), E(cm)=643, 420 MeV; 208Pb(136Xe, X), E(cm)=450, 526 MeV; 186W(136Xe, X), E(cm)=408 MeV; 186W(150Nd, X), E(cm)=451 MeV; calculated potential energy surfaces, total kinetic energy losses (TKEL), and production σ with and without shell corrections using dinuclear system (DNS) model; deduced shell effects on producing trans-target nuclei. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.044614
2018ZH39 Phys.Rev. C 98, 034609 (2018) L.Zhu, J.Su, P.-W.Wen, C.-C.Guo, C.Li Multinucleon transfer process in the reaction 160Gd + 186W NUCLEAR REACTIONS 186W(160Gd, X), E(cm)=430, 450, 503, 550 MeV; calculated potential energy surface as a function of mass asymmetry and β2 deformation, σ(E) for production of primary products as function of mass number, TKEL and β2, N/Z distribution of primary products, and production σ(E) of Os and Np isotopes, 202Os, 201Re, 240Np, 241U, and isotopes of Z=60-100, N=90-150. Dinuclear system (DNS) model with GEMINI code for multinucleon transfer (MNT) process.
doi: 10.1103/PhysRevC.98.034609
2017SU23 Phys.Rev. C 96, 024601 (2017) J.Su, L.Zhu, C.-Y.Huang, W.-J.Xie, F.-S.Zhang Effects of symmetry energy and effective k-mass splitting on central 96Ru(96Zr) + 96Zr(96) collisions at 50 to 400 MeV/nucleon NUCLEAR REACTIONS 96Ru(96Zr, X), 96Zr(96Ru, X), E=50-400 MeV/nucleon; calculated slope and quantum temperatures, np, nn, and pp collisions as a function of time, observable n/p ratio from the free neutrons and protons as a function of rapidity; investigated isospin mixing in central heavy-ion collisions (HICs). Isospin-dependent quantum molecular dynamics model in combination with the statistical decay code GEMINI. Comparison with experimental data from FOPI Collaboration.
doi: 10.1103/PhysRevC.96.024601
2017YA27 Astrophys.J. 848, 98 (2017) S.Q.Yan, Z.H.Li, Y.B.Wang, K.Nishio, M.Lugaro, A.I.Karakas, H.Makii, P.Mohr, J.Su, Y.J.Li, I.Nishinaka, K.Hirose, Y.L.Han, R.Orlandi, Y.P.Shen, B.Guo, S.Zeng, G.Lian, Y.S.Chen, W.P.Liu The 95Zr(n, γ)96Zr Cross Section from the Surrogate Ratio Method and Its Effect on s-process Nucleosynthesis NUCLEAR REACTIONS 94,90Zr(18O, 16O), E=117 MeV; measured reaction products; deduced σ for surrogate reactions. Comparison with KADONIS and ENDF/B-VII.1 evaluated nuclear library and TALYS nuclear code calculations.
doi: 10.3847/1538-4357/aa8c74
2017ZH19 Phys.Rev. C 95, 044608 (2017) Optimal incident energies for production of neutron-deficient actinide nuclei in the reaction 58Ni + 238U NUCLEAR REACTIONS 238U(58Ni, X)216Np/217Np/218Np/219Np/222Np/224Np/226Np/228Np/230Np/232Np/234Np/236Np/238Np/240Np, E(cm)=260-400 MeV; calculated production σ(E) for A=216-240 Np isotopes. 222,223,224,225,226,227Pu, 224,225,226,227,228,231Am, 228,229,230,231,232Cm, 230,231,232,235,236,237Bk; predicted optimal incident energies (OPEs) for producing unknown neutron-deficient isotopes with Z=9497 in 58Ni+238U transfer reaction. Dinuclear system model.
doi: 10.1103/PhysRevC.95.044608
2017ZH21 Nucl.Phys. A964, 93 (2017) Theoretical predictions on production of neutron-deficient nuclei with Z ≥ 93 in multinucleon transfer reactions NUCLEAR REACTIONS 233U(58Ni, x), E(cm)=1.2, 1.3, 1.4 Coulomb barrier;238U(58Ni, x), (64Ni, x), E(cm)=1.3 Coulomb barrier;245Cm(40Ca, x), E(cm)=1.2, 1.3, 1.4 Coulomb barrier; calculated production σ of some neutron-deficient actinide isotopes; deduced feasible ways to produce neutron-deficient actinide nuclei in future.
doi: 10.1016/j.nuclphysa.2017.05.063
2017ZH32 Phys.Rev. C 96, 024606 (2017) L.Zhu, F.-S.Zhang, P.-W.Wen, J.Su, W.-J.Xie Production of neutron-rich nuclei with Z=60-73 in reactions induced by Xe isotopes NUCLEAR REACTIONS 238U(136Xe, X), E(cm)=636 MeV; calculated production σ for A=122-150 Ba, Cs, Te and I isotopes, and compared with experimental data. 238U(124Xe, X), (136Xe, X), (144Xe, X), E(cm)=473-493 MeV; calculated production σ for target-like fragments (TLFs) with A=206-250, Z=88-96 neutron-rich isotopes, PES as functions of Z and N in 144Xe+238U reaction, yield distributions of total primary fragments as a function of their N/Z ratio for 124Xe+238U and 144Xe+238U reactions. 160Gd, 170Er, 186W(136Xe, X), (144Xe, X), E(cm)=353-406 MeV; calculated production σ for A=140-190, Z=60-73 neutron-rich isotopes. Dinuclear system model.
doi: 10.1103/PhysRevC.96.024606
2016LI51 Chin.Phys.C 40, 114104 (2016) E.T.Li, B.Guo, Z.H.Li, Y.B.Wang, Y.J.Li, Z.D.Wu, J.Su, D.Y.Pang, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, X.Hao, S.P.Hu, J.J.He, L.Jing, S.J.Jin, L.Li, X.Y.Li, Z.C.Li, G.Lian, J.C.Liu, Q.Luo, L.H.Qiao, Y.P.Shen, H.B.Sun, S.Q.Yan, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, Y.Zhou, W.P.Liu Radii of the bound states in 16N from the asymptotic normalization coefficients RADIOACTIVITY 16N(n) [from 15N(7Li, 6Li)16N, E=44 MeV]; analyzed available data; deduced asymptotic normalization coefficients (ANCs), rms radii of the valence neutron, probabilities of the valence neutron staying out of the core potentials.
doi: 10.1088/1674-1137/40/11/114104
2016SU10 Phys.Lett. B 756, 323 (2016) J.Su, W.P.Liu, N.T.Zhang, Y.P.Shen, Y.H.Lam, N.A.Smirnova, M.MacCormick, J.S.Wang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, Z.C.Gao, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li, G.Audi Revalidation of the isobaric multiplet mass equation at A = 53, T = 3/2 RADIOACTIVITY 53Ni(EC), (ECp) [from Be(58Ni, X)53Ni, E=68.3 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced T1/2, level scheme, J, π, isobaric analog state, mass excess, explanation of unexpected deviation from the isobaric multiplet mass equation (IMME) at A=53, T=3/2.
doi: 10.1016/j.physletb.2016.03.024
2016SU18 Eur.Phys.J. A 52, 207 (2016) J.Su, C.-Y.Huang, W.-J.Xie, F.-S.Zhang Effects of in-medium nucleon-nucleon cross sections on stopping observable and ratio of free protons in heavy-ion collisions at 400 MeV/nucleon NUCLEAR REACTIONS 96Zr, 96Ru(96Ru, x), E=400 MeV/nucleon; calculated in-medium factors vs energy and vs density using IQMD (Isospin-dependent Quantum Molecular Dynamics); deduced isospin effect using comparison with data.
doi: 10.1140/epja/i2016-16207-x
2016SU21 Phys.Rev. C 94, 034619 (2016) J.Su, L.Zhu, C.-Y.Huang, W.-J.Xie, F.-S.Zhang Correlation between symmetry energy and effective k-mass splitting with an improved isospin- and momentum-dependent interaction NUCLEAR REACTIONS 124Sn(124Sn, X), 112Sn(112Sn, X), E=50, 120 MeV/nucleon; analyzed double ratios of the coalescence invariant neutron and proton spectra in central collisions; extracted isospin transport ratios from the yield ratios of A=7 isotopes using IQMD+GEMINI model.
doi: 10.1103/PhysRevC.94.034619
2016SU22 Yuan.Wul.Ping. 33, 230 (2016); Nucl.Phys.Rev. 33, 230 (2016) L.Sun, X.Xu, C.Lin, J.Wang, D.Fang, Z.Li, Y.Wang, J.Li, L.Yang, N.Ma, K.Wang, H.Zhang, H.Wang, C.Li, C.Shi, M.Nie, X.Li, H.Li, J.Ma, P.Ma, S.Jin, M.Huang, Z.Bai, J.Wang, F.Yang, H.Jia, H.Zhang, Z.Liu, P.Bao, S.Wang, Z.Wu, Y.Yang, Z.Chen, J.Su, Y.Shen, Y.Zhou, W.Ma, J.Chen An implantation and detection system for spectroscopy of 22, 24Si RADIOACTIVITY 22,24Si(β+p); measured decay products, Ep, Ip; deduced energy levels, J, π, T1/2, branchning ratios.
doi: 10.11804/NuclPhysRev.33.02.230
2016WA18 Phys.Rev. C 94, 024608 (2016) Y.Wang, C.Guo, Q.Li, Z.Li, J.Su, H.Zhang Influence of differential elastic nucleon-nucleon cross section on stopping and collective flow in heavy-ion collisions at intermediate energies NUCLEAR REACTIONS 1H(p, p), (n, n), E=150, 250, 400, 800 MeV; calculated normalized NN differential cross sections versus the cosine of the center-of-mass scattering angle, and compared with experimental data at ≈400 MeV. 197Au(197Au, X), E=150, 250, 400, 800 MeV/nucleon; calculated longitudinal and transverse rapidity distributions, directed and elliptic flows of free protons using three nucleon-nucleon (NN) elastic differential cross sections: parameterized differential cross section, differential cross section from the collision term of the self-consistent relativistic Boltzmann-Uehling-Uhlenbeck equation, and the isotropic differential cross section within the new version of the ultrarelativistic quantum molecular dynamics (UrQMD) model.
doi: 10.1103/PhysRevC.94.024608
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
2016YA09 Phys.Rev. C 94, 015804 (2016) S.Q.Yan, Z.H.Li, Y.B.Wang, K.Nishio, H.Makii, J.Su, Y.J.Li, I.Nishinaka, K.Hirose, Y.L.Han, R.Orlandi, Y.P.Shen, B.Guo, S.Zeng, G.Lian, Y.S.Chen, X.X.Bai, L.H.Qiao, W.P.Liu Examination of the surrogate ratio method for the determination of the 93Zr (n, γ)94Zr cross section with 90, 92Zr(18O, 16O) 92, 94Zr reactions NUCLEAR REACTIONS 90,92Zr(18O, 16O), E=117 MeV; measured Eγ, Iγ, (16O)γ-coin at the Tandem accelerator of JAEA facility. 92,94Zr; measured γ-decay probability ratios. 93Zr(n, γ), E>3 MeV; deduced σ(E) by surrogate ratio method, using reference cross sections of the 91Zr(n, γ)92Zr reaction from ENDF/B-VII.1, and the measured γ-decay probability ratios.
doi: 10.1103/PhysRevC.94.015804
2016ZH23 Phys.Rev. C 93, 064610 (2016) Influence of the neutron numbers of projectile and target on the evaporation residue cross sections in hot fusion reactions NUCLEAR REACTIONS 238U(34S, 3n)269Hs, 238U(34S, 4n)268Hs, 238U(34S, 5n)267Hs, 238U(36S, 3n)272Hs, 238U(36S, 4n)271Hs, 238U(36S, 5n)270Hs, E(cm)=140-210 MeV; 238Pu(48Ca, 3n)283Fl, 238Pu(48Ca, 4n)282Fl, 238Pu(48Ca, 5n)281Fl, 239Pu(48Ca, 3n)284Fl, 239Pu(48Ca, 4n)283Fl, 240Pu(48Ca, 3n)285Fl, 240Pu(48Ca, 4n)284Fl, 242Pu(48Ca, 2n)288Fl, 242Pu(48Ca, 3n)287Fl, 242Pu(48Ca, 4n)286Fl, 242Pu(48Ca, 5n)285Fl, 244Pu(48Ca, 3n)289Fl, 244Pu(48Ca, 4n)288Fl, 244Pu(48Ca, 5n)287Fl, 244Pu(42Ca, 3n)283Fl, 244Pu(42Ca, 4n)282Fl, 244Pu(42Ca, 5n)281Fl, 244Pu(43Ca, 3n)284Fl, 244Pu(43Ca, 4n)283Fl, 244Pu(43Ca, 5n)282Fl, 244Pu(44Ca, 3n)285Fl, 244Pu(44Ca, 4n)284Fl, 244Pu(44Ca, 5n)283Fl, 244Pu(46Ca, 3n)287Fl, 244Pu(46Ca, 4n)286Fl, 244Pu(46Ca, 5n)285Fl, 238U(44Ca, 3n)279Cn, 238U(44Ca, 4n)278Cn, 238U(44Ca, 5n)277Cn, 242Pu(44Ca, 3n)283Fl, 242Pu(44Ca, 4n)282Fl, 242Pu(44Ca, 5n)281Fl, 248Cm(44Ca, 3n)289Lv, 248Cm(44Ca, 4n)288Lv, 248Cm(44Ca, 5n)287Lv, 238U(46Ca, 3n)281Cn, 238U(46Ca, 4n)280Cn, 238U(46Ca, 5n)279Cn, 237Np(46Ca, 3n)280Nh, 237Np(46Ca, 4n)279Nh, 237Np(46Ca, 5n)278Nh, 239Pu(46Ca, 3n)282Fl, 239Pu(46Ca, 4n)281Fl, 239Pu(46Ca, 5n)280Fl, 240Pu(46Ca, 3n)283Fl, 240Pu(46Ca, 4n)282Fl, 240Pu(46Ca, 5n)281Fl, 241Am(46Ca, 3n)284Mc, 241Am(46Ca, 4n)283Mc, 241Am(46Ca, 5n)282Mc, 243Am(46Ca, 3n)286Mc, 243Am(46Ca, 4n)285Mc, 243Am(46Ca, 5n)284Mc, 243Cm(46Ca, 3n)286Lv, 243Cm(46Ca, 4n)285Lv, 243Cm(46Ca, 5n)284Lv, 245Cm(46Ca, 3n)288Lv, 245Cm(46Ca, 4n)287Lv, 245Cm(46Ca, 5n)286Lv, 235U(48Ca, 3n)280Cn, 235U(48Ca, 4n)279Cn, 235U(48Ca, 5n)278Cn, 241Am(48Ca, 3n)286Mc, 241Am(48Ca, 4n)285Mc, 241Am(48Ca, 5n)284Mc, 243Cm(48Ca, 3n)289Lv, 243Cm(48Ca, 4n)288Lv, 243Cm(48Ca, 5n)287Lv; Calculated evaporation residues (ER) cross sections for superheavy elements, and compared with available experimental data. Maximum cross sections deduced for 243Cm(46Ca, 3n)288Lv, E(cm)=200.7 MeV, 241Am(48Ca, 4n)285Mc, E(cm)=210.5 MeV, 248Cm(44Ca, 4n)288Lv, E(cm)=201.7 MeV, and 238Pu(48Ca, 4n)282Fl, E(cm)=208.7 MeV. Dinuclear system model.
doi: 10.1103/PhysRevC.93.064610
2016ZH48 Phys.Rev. C 94, 054606 (2016) L.Zhu, J.Su, W.-J.Xie, F.-S.Zhang Production of neutron-rich transcalifornium nuclei in 238U-induced transfer reactions NUCLEAR REACTIONS 248Cm(238U, X), E(cm)=800 MeV; calculated production σ for A=248-254 Es, Fm and Md isotopes, and compared with experimental data. 248,250Cm, 249Cf, (238U, X), E(cm)=1.1(VCN=interaction potential at the touching point); calculated production σ for A=245-270 Es, Fm, Md, No, Lr and Rf isotopes. Dinuclear system (DNS) model.
doi: 10.1103/PhysRevC.94.054606
2016ZH50 Chin.Phys.C 40, 124105 (2016) L.Zhu, J.Su, C.-Y.Huang, F.-S.Zhang Effects of entrance channel on fusion probability in hot fusion reactions NUCLEAR REACTIONS 248Cm(26Mg, X)274Hs, 238U(36S, X)274Hs, 226Ra(48Ca, X)274Hs, E<60 MeV/nucleon; 238U(48Ca, X)286Cn, 234U(52Ca, X)286Cn, 231Pa(55Sc, X)286Cn, E<60 MeV/nucleon; analyzed available data; calculated fusion probability as a function of dinuclear system excitation energy. Comparison with available data.
doi: 10.1088/1674-1137/40/12/124105
2015SH16 Phys.Rev. C 91, 047304 (2015) Y.P.Shen, W.P.Liu, J.Su, N.T.Zhang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, J.S.Wang, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li Measurement of the 52Fe mass via the precise proton-decay energy of 53Com RADIOACTIVITY 53mCo(p)[from 9Be(58Ni, X), E=68.3 MeV/nucleon]; 41Ti(β+p); measured Ep, Ip, at RIBLL-HIRFL-Lanzhou facility; deduced mass excess of 52Fe and compared with AME-2012 evaluation. 51Fe, 52Co(β+); measured half-lives and compared with evaluated data in ENSDF. ATOMIC MASSES 52Fe; deduced mass excess from Q value of proton decay of 3174.1 keV, 19/2- isomer in 53Co determined from measured proton energy. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.047304
2015XI01 Phys.Rev. C 91, 054609 (2015) W.-J.Xie, Z.-Q.Feng, J.Su, F.-S.Zhang Probing the momentum-dependent symmetry potential via nuclear collective flows NUCLEAR REACTIONS 197Au(197Au, X), E=250-800 MeV/nucleon; calculated directed and elliptic flow of protons, rapidity and transverse momentum dependence of the neutron-proton differential directed flow. Isospin-dependent quantum molecular dynamics (IQMD) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.054609
2015ZH11 Chin.Phys.C 39, 044103 (2015) D.-H.Zhang, W.-J.Xie, J.Su, F.-S.Zhang Production cross section of neutron-rich calcium isotopes in heavy ion collisions NUCLEAR REACTIONS 112Sn(112Sn, X), 124Sn(124Sn, X)48Ca/54Ca, E<160 MeV; calculated production σ. IQMD+GEMINI model.
doi: 10.1088/1674-1137/39/4/044103
2014CH05 Phys.Rev. C 89, 014618 (2014) K.Cherevko, L.Bulavin, J.Su, V.Sysoev, F.-S.Zhang "Doughnut" nuclear shapes in head-on heavy ion collisions
doi: 10.1103/PhysRevC.89.014618
2014GU02 Phys.Rev. C 89, 012801 (2014) B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, Z.D.Wu, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, L.Y.Zhang, W.J.Zhang, W.P.Liu Spectroscopic factors for low-lying 16N levels and the astrophysical 15N(n, γ)16N NUCLEAR REACTIONS 15N(7Li, 6Li)16N, E=44 MeV; measured 6Li spectrum, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA analysis. Comparison with shell model calculations. 15N(n, γ)16N, at T=0.01-3 GK; deduced astrophysical reaction rates. Comparison with previous experimental and theoretical results.
doi: 10.1103/PhysRevC.89.012801
2014HU16 Phys.Rev. C 90, 025803 (2014) J.Hu, J.J.He, A.Parikh, S.W.Xu, H.Yamaguchi, D.Kahl, P.Ma, J.Su, H.W.Wang, T.Nakao, Y.Wakabayashi, T.Teranishi, K.I.Hahn, J.Y.Moon, H.S.Jung, T.Hashimoto, A.A.Chen, D.Irvine, C.S.Lee, S.Kubono Examination of the role of the 14O(α, p)17F reaction rate in type-I x-ray bursts NUCLEAR REACTIONS 1H(17F, p), E=3.6 MeV/nucleon, [17F secondary beam from 2H(16O, n), E=6.6 MeV/nucleon primary reaction]; measured Ep, Ip, angular distribution using radioactive ion beam separator (CRIB) at CNS-RIKEN facility. 18Ne; deduced levels, resonances, J, π, L-transfers, widths, proton partial widths, resonance strengths. R-matrix analysis of experimental data. Comparison with previous experimental results. 14O(α, p)17F, at T9=0.25-3.0; deduced reaction rates and compared with other studies. Relevance to hot-CNO cycle of the rp-process in type-I x-ray bursts (XRBs).
doi: 10.1103/PhysRevC.90.025803
2014LI49 Phys.Rev. C 90, 067601 (2014) E.T.Li, Z.H.Li, Y.J.Li, B.Guo, Y.B.Wang, D.Y.Pang, J.Su, S.Q.Yan, S.Zeng, L.Gan, Z.C.Li, J.C.Liu, X.X.Bai, Z.D.Wu, S.J.Jin, L.Y.Zhang, X.Q.Yu, L.Li, H.B.Sun, G.Lian, Q.W.Fan, W.P.Liu Proton spectroscopic factor of the 12C ground state from the 12C(11B, 12C) 11B elastic transfer reaction NUCLEAR REACTIONS 12C(11B, 11B), (11B, 12C)11B, E=50 MeV; measured particle spectra, angular distributions using Q3D magnetic spectrometer at the HI-13 tandem accelerator of CIAE facility. 12C; deduced optical potential parameters, proton spectroscopic factor for 12C g.s., DWBA calculations. Comparison with previous experimental and theoretical results.
doi: 10.1103/PhysRevC.90.067601
2014SU03 Phys.Rev. C 89, 014619 (2014) J.Su, K.Cherevko, W.-J.Xie, F.-S.Zhang Nonisotropic and nonsingle explosion in central 129Xe + 120Sn collisions at 50-125 MeV/nucleon NUCLEAR REACTIONS 129Xe(120Sn, X), E=50-125 MeV/nucleon; calculated average kinetic energy, average multiplicity of fragments as a function of charge for forward and sideward angles, collective and Coulomb expansion energy per nucleon as a function of polar angle, radial flow energies of H, He, Li, and Be fragments, contours of time evolutions of the density and the collective velocity, longitudinal and transverse collective velocity as a function of radius. Isospin-dependent quantum molecular dynamics model, and statistical decay code GEMINI. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.014619
2014WU03 Phys.Rev. C 89, 054315 (2014) Z.D.Wu, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, W.P.Liu Proton widths of the low-lying 16F states from the 15N(7Li, 6Li)16N reaction NUCLEAR REACTIONS 15N(7Li, 7Li), (7Li, 6Li), E=34.5, 44 MeV; measured particle spectra, elastic and inelastic σ(θ) using Q3D magnetic spectrograph at CIAE facility. 16N; deduced levels, J, π, asymptotic normalization coefficients (ANCs), spectroscopic factors. DWBA analysis. 16F; deduced proton and single-particle widths, spectroscopic factors for first four levels from mirror analogy with 16N. Comparison with previous experimental results and compilation.
doi: 10.1103/PhysRevC.89.054315
2013GU04 Phys.Rev. C 87, 015803 (2013) B.Guo, J.Su, Z.H.Li, Y.B.Wang, S.Q.Yan, Y.J.Li, N.C.Shu, Y.L.Han, X.X.Bai, Y.S.Chen, W.P.Liu, H.Yamaguchi, D.N.Binh, T.Hashimoto, S.Hayakawa, D.Kahl, S.Kubono, J.J.He, J.Hu, S.W.Xu, N.Iwasa, N.Kume, Z.H.Li Determination of the astrophysical 12N(p, γ)13O reaction rate from the 2H(12N, 13O)n reaction and its astrophysical implications NUCLEAR REACTIONS 2H(12N, 13O)1n, E=59 MeV; measured reaction products, energy loss, time-of-flight, differential σ(θ); deduced ANC, astrophysical S factors. 12N(p, γ)13O, at T9=0.3-3.0; deduced stellar reaction rate. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.87.015803
2013JI13 Phys.Rev. C 88, 035801 (2013) S.J.Jin, Y.B.Wang, J.Su, S.Q.Yan, Y.J.Li, B.Guo, Z.H.Li, S.Zeng, G.Lian, X.X.Bai, W.P.Liu, H.Yamaguchi, S.Kubono, J.Hu, D.Kahl, H.S.Jung, J.Y.Moon, C.S.Lee, T.Teranishi, H.W.Wang, H.Ishiyama, N.Iwasa, T.Komatsubara, B.A.Brown Resonant scattering of 22Na+p studied by the thick-target inverse-kinematic method NUCLEAR REACTIONS 1H(22Na, 22Na), E<37.1 MeV, [22Na secondary beam from 1H(22Ne, 22Na), E=6.0 MeV/nucleon primary reaction]; measured back-angle recoil-proton spectra, TOF, differential σ(E) using thick target technique at RIBF-RIKEN facility. R-matrix analysis of resonance spectra. 23Mg; deduced levels, resonances, J, π, Γp, Γγ, resonance strengths, two s-wave resonances. Comparison with previous experimental data, and with shell-model calculations. 22Na(p, γ)23Mg, T9=0.01-10; deduced astrophysical reaction rates. Comparison with previous experimental data and NACRE evaluation. NUCLEAR STRUCTURE 23Mg; calculated levels, J, π, s-wave resonances, their spectroscopic factors and γ widths using shell model with usda and usdb interactions. Comparison with experimental data, and with structure of 23Na mirror nucleus.
doi: 10.1103/PhysRevC.88.035801
2013LI09 Phys.Rev. C 87, 017601 (2013) Z.H.Li, Y.J.Li, J.Su, B.Guo, E.T.Li, K.J.Dong, X.X.Bai, Z.C.Li, J.C.Liu, S.Q.Yan, Y.B.Wang, S.Zeng, G.Lian, B.X.Wang, S.J.Jin, X.Liu, W.J.Zhang, W.Z.Huang, Q.W.Fan, L.Gan, Z.D.Wu, W.P.Liu New determination of the proton spectroscopic factor in 9Be from the 13C(9Be, 8Li)14N angular distribution NUCLEAR REACTIONS 13C(9Be, 8Li)14N, 12,13C(9Be, 9Be), E=40 MeV; measured particle spectra, Eα, differential s(θ) using Q3D magnetic spectrometer at HI-13 tandem accelerator facility in Beijing. 9Be; deduced proton spectroscopic factor for g.s. Optical model and DWBA analysis. Comparison with previous experimental and theoretical studies. Relevance to astrophysical S factor for 8Li(p, γ)9Be reaction.
doi: 10.1103/PhysRevC.87.017601
2013SU03 Phys.Rev. C 87, 017602 (2013) Non-equilibrium and residual memory in momentum space of fragmenting sources in central heavy-ion collisions
doi: 10.1103/PhysRevC.87.017602
2013SU07 Phys.Rev. C 87, 024312 (2013) J.Su, W.P.Liu, N.C.Shu, S.Q.Yan, Z.H.Li, B.Guo, W.Z.Huang, S.Zeng, E.T.Li, S.J.Jin, X.Liu, Y.B.Wang, G.Lian, Y.J.Li, Y.S.Chen, X.X.Bai, J.S.Wang, Y.Y.Yang, R.F.Chen, S.W.Xu, J.Hu, S.Z.Chen, S.B.Ma, J.L.Han, P.Ma, Q.Hu, J.B.Ma, X.G.Cao, S.L.Jin, Z.Bai, K.Yang, F.D.Shi, W.Zhang, Z.Chen, L.X.Liu, Q.Y.Lin, X.S.Yan, X.H.Zhang, F.Fu, J.J.He, X.Q.Li, C.He, M.S.Smith Reexamining the β decay of 53, 54Ni, 52, 53Co, 51Fe, and 50Mn RADIOACTIVITY 50Mn, 50Cr, 51Fe, 52,53Co, 53,54Ni(β+), (EC), (β+p)[from (58Ni, X), E=68.6 MeV/nucleon]; measured β-delayed protons, (proton)γ-coin, Eγ, Iγ, T1/2 at HIRFL facility in Lanzhou. Implications for r process. Comparison with previous experimental studies.
doi: 10.1103/PhysRevC.87.024312
2013XI13 Phys.Rev. C 88, 061601 (2013) W.-J.Xie, J.Su, L.Zhu, F.-S.Zhang Neutron-proton effective mass splitting in a Boltzmann-Langevin approach
doi: 10.1103/PhysRevC.88.061601
2013ZH36 Nucl.Phys. A915, 90 (2013) L.Zhu, J.Su, W.-J.Xie, F.-S.Zhang Study of the dynamical potential barriers in heavy ion collisions NUCLEAR REACTIONS 58Ni(58Ni, X), E(cm)=94-110 MeV;64Ni(64Ni, X), E(cm)=90-109 MeV;154Sm(16O, X), E(cm)=52-90 MeV;208Pb(16O, X), E(cm)=72-280 MeV; calculated fusion σ using isospin-dependent QMD with shell corrections; deduced relative orientation of nuclei, nucleus-nucleus potentials. Compared to data.
doi: 10.1016/j.nuclphysa.2013.07.003
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