NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = Shen Qingbiao Found 61 matches. 2020CH49 J.Phys.(London) G47, 025106 (2020) W.Chen, H.Guo, W.Sun, T.Ye, Y.J.Ying, Y.Han, Q.Shen Microscopic optical potential for 7Li NUCLEAR REACTIONS 40,44,48Ca, 56Fe, 60,62Ni, 64,68Zn, 90Zr, 46,48Ti, 140Ce, 142Nd, 28Si, 80Se, 120Sn, 144Sm, 208Pb(7Li, X), E<100 MeV; calculated σ(θ), σ. Comparison with available data.
doi: 10.1088/1361-6471/ab52d3
2018XU03 Int.J.Mod.Phys. E27, 1850023 (2018) The proton microscopic optical potential based on Skyrme interaction NUCLEAR REACTIONS 54,56Fe, 51V, 40Ca, 28Si, 27Al, 59Co, 58,60Ni, 63Cu, 90Zr, 120Sn, 208Pb, 232Th, 238U(p, p), E<100 MeV; calculated σ, σ(θ). Comparison with available data.
doi: 10.1142/S0218301318500234
2017GU06 Phys.Rev. C 95, 034614 (2017) H.Guo, H.Liang, Y.Xu, Y.Han, Q.Shen, C.Cai, T.Ye Microscopic optical potential for 6He NUCLEAR REACTIONS 12C(6He, 6He), E=8.79, 9.18, 9.9, 18, 230, 250 MeV; 27Al(6He, 6He), E=9.54, 11.0, 12.0, 13.4 MeV; 51V(6He, 6He), E=15.4, 23.0 MeV; 58Ni(6He, 6He), E=9.0, 10.0, 12.2, 16.5, 21.7 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 65Cu(6He, 6He), E=19.56, 22.6, 30.05 MeV; 120Sn(6He, 6He), E=17.4, 18.05, 19.8, 20.05 MeV; 197Au(6He, 6He), E=10.1, 27.0 MeV; 209Bi(6He, 6He), E=14.71, 16.26, 17.8, 19.0, 19.14, 22.02, 22.5 MeV; 208Pb(6He, 6He), E=14.0, 16, 18, 22, 27, 56.6 MeV; 9Be(6He, 6He), E=16.2, 16.8, 21.3, 150 MeV; calculated differential σ(θ, E) relative to Rutherford cross section using microscopic optical potential (MOP) and global phenomenological 6He optical potential (GOP) based on experimental data. 28Si(6He, X), E<330 MeV; calculated total σ(E) using MOP and GOP. Comparison with experimental data. Isospin-dependent nucleon microscopic optical potential derived by using Green's function method through the nuclear matter approximation and the local density approximation based on the Skyrme nucleon-nucleon effective interaction.
doi: 10.1103/PhysRevC.95.034614
2017GU11 Nucl.Sci.Eng. 186, 156 (2017) H.Guo, Y.Xu, Y.Han, Q.Shen, T.Ye, W.Sun Calculation and Evaluation for the n+51V Reaction NUCLEAR REACTIONS 51V(n, n), E<300 MeV; calculated σ, σ(E), σ(θ), σ(θ, E). Optical model, distorted wave Born approximation theory, Hauser-Feshbach theory, evaporation model, exciton model, and intranuclear cascade model, comparison with the experimental data and the evaluated results in ENDF/B-VII.1 and JENDL-4 libraries.
doi: 10.1080/00295639.2016.1273008
2017XU05 Phys.Rev. C 96, 024621 (2017) New extended Skyrme interaction for nuclear properties and nuclear reactions NUCLEAR STRUCTURE 16O, 40,48Ca, 56,60Ni, 88Sr, 90Zr, 114Sn, 146Gd, 204Hg, 206,208Pb; calculated relative deviations of charge radii and energies per nucleon using SkC17, SkC, and GS2 Skyrme interactions. 208Pb; calculated neutron and proton single-particle energy levels near the Fermi surface using various Skyrme interactions, and compared with experimental data. NUCLEAR REACTIONS 56Fe, 208Pb(n, X), E=0.1-100 MeV; calculated total and non-elastic σ(E) using SkC17, SkC, GS2, and SkOP4 Skyrme interactions, and compared with experimental data. 24Mg, 54,58Fe, 59Co, 90Zr, 93Nb, 92,96,98,100Mo, 120Sn, 206,208Pb(n, n), E=11.0 MeV; 28Si, 40Ca, 56Fe, 90Zr, 120Sn, 208Pb(n, n), E=65.0 MeV; 56Fe, 208Pb(n, n), E=1.68-96.0 MeV; 100Mo(n, n), E=0.34-26.0 MeV; 12C(n, n), E=0.5-94.8 MeV; 238U(n, n), E=4.5=10 MeV; 181Ta(n, n), E=0.32-15.2 MeV; 54Fe(polarized n, n), E=9.94, 13.92, 16.93 MeV; 89Y(polarized n, n), E=9.95, 13.93, 16.93 MeV; 208Pb(polarized n, n), E=5.97, 6.97, 7.96, 8.96, 9.95, 13.9, 23.0 MeV;calculated σ(θ, E), analyzing powers using different Skyrme interaction parameters; deduced SkC17 Skyrme interaction by simultaneously fitting variety of experimental data. Extended Skyrme interaction involving additional momentum- and density-dependent terms.
doi: 10.1103/PhysRevC.96.024621
2017XU09 Int.J.Mod.Phys. E26, 1750065 (2017) Isospin dependence of the nucleon density distributions NUCLEAR STRUCTURE 40,48Ca, 124Sn, 208Pb; calculated proton density distributions, rms radii. Comparison with available data.
doi: 10.1142/S0218301317500653
2014GU01 Nucl.Phys. A922, 84 (2014) H.Guo, Y.Xu, H.Liang, Y.Han, Q.Shen Microscopic optical model potential for triton NUCLEAR REACTIONS A=6-232(t, t), (t, X), E=threshold-60 MeV/nucleon; calculated triton microscopic optical model potential, reaction σ, elastic scattering σ(θ). Compared with some data.
doi: 10.1016/j.nuclphysa.2013.11.007
2014HA16 Nucl.Data Sheets 118, 108 (2014) Y.Han, C.Cai, H.Guo, Z.Zhang, Q.Shen Present Status of Evaluated Nuclear Data Library for ADS in China COMPILATION 27Al(n, x), E=0.01-350 MeV; calculated σ. 27Al(n, xn), E=14.1 MeV; calculated σ(En, θ). 27Al(n, xp), (n, xn), E=≈30-62.7 MeV; calculated σ(Eout). 27Al(n, 3He), E=95.6 MeV; calculated σ(Eout, θ). 209Bi(p, 3n), (p, 2np), E=20-200 MeV; calculated σ. 209Bi(p, x), E=61.7 MeV; calculated σ(Eout, θ). UNF code (optical model plus unified HF plus exciton model); compared with data.
doi: 10.1016/j.nds.2014.04.012
2014HA17 Nucl.Data Sheets 118, 132 (2014) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculation of Actinide Nuclear Reaction Data
doi: 10.1016/j.nds.2014.04.018
2014LI10 Ann.Nucl.Energy 69, 301 (2014) The energy spectra and double-differential cross-sections for p+92, 94, 95, 96, 97, 98, 100Mo reactions at the incident energies from threshold to 200 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, xn), (p, xp), (p, xd), (p, xα), (p, xt), E<160 MeV; calculated σ(E), σ(E, θ). Exciton model including the improved Iwamoto-Harada model, comparison with experimental data.
doi: 10.1016/j.anucene.2014.02.008
2014XU01 J.Phys.(London) G41, 015101 (2014) New Skyrme interaction parameters for a unified description of the nuclear properties NUCLEAR REACTIONS 28Si, 56Fe, 208Pb(n, X), (n, n), 27Al, 90Zr, 208Pb, 232Th(p, p), E<100 MeV; calculated σ, σ(θ). Skyrme-Hartree-Fock approach, comparison with available data.
doi: 10.1088/0954-3899/41/1/015101
2013HA04 Ann.Nucl.Energy 55, 75 (2013) Double differential cross sections of light charged particle emission of n + 27Al reaction NUCLEAR REACTIONS 27Al(n, xp), (n, xd), (n, xt), (n, xα), (n, 3He), E<40 MeV; calculated σ(E, θ), σ(E). Comparison with available data.
doi: 10.1016/j.anucene.2012.11.031
2012HA16 Ann.Nucl.Energy 46, 179 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen The analysis of n+237Np reactions for energies up to 200 MeV NUCLEAR REACTIONS 237Np(n, γ), (n, F), (n, 2n), (n, xn), (n, xp), (n, xd), (n, xt), (n, xα) E<200 MeV; calculated σ, σ(θ, E), σ(θ), σ(E). Optical model, the intra-nuclear cascade model, the unified Hauser-Feshbach theory, comparison with ENDF/B-VII and JENDL-3 libraries and available data.
doi: 10.1016/j.anucene.2012.03.013
2012HA24 Nucl.Sci.Eng. 172, 102 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculations and Analysis of n + 27Al Reaction NUCLEAR REACTIONS 27Al(n, X), (n, n), (n, n'), (n, p), (n, γ), (n, d), (n, t), (n, α), (n, 2n), (n, xn), (n, xp), (n, xα), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Comparison with ENDF/B-VII and JENDL-3 evaluated nuclear libraries.
doi: 10.13182/NSE11-28
2011GU15 Phys.Rev. C 83, 064618 (2011) H.Guo, Y.Xu, H.Liang, Y.Han, Q.Shen 4He microscopic optical model potential NUCLEAR REACTIONS 12C, 58Ni, 116Sn, 208Pb(α, X), E=20-300 MeV; calculated radial dependence of real and imaginary parts of the potential, volume integral and rms radii. 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb, 209Bi(α, X), E=5-200 MeV; calculated reaction σ(E). 62,64Ni, 63,65Cu, 64,66,68,70Zn, 70,72Ge(α, α), E=25.0 MeV; 94Mo, 107Ag, 116,122,124Sn(α, α), E=25.2 MeV; 20,22Ne, 24,26Mg, 28Si, 40Ar, 40,42,44,48Ca, 56Fe, 56,58,60,62Ni, 90Zr, 124Sn, 208Pb(α, α), E=104 MeV; 16O, 46,48Ti, 58Ni, 116Sn, 197Au(α, α), E=240 MeV; 12C, 58Ni, 90Zr, 116Sn, 144Sm, 208Pb(α, α), E=386.0 MeV; calculated σ(θ). 12C(α, α), E=120.0-400 MeV; 58Ni(α, α), E=29.0-386 MeV; 24Mg(α, α), E=39.0-172.5 MeV; 107Ag(α, α), E=15.0-43.0 MeV; 116Sn(α, α), E=23.3-386 MeV; 124Sn(α, α), E=23.3-104 MeV; 208Pb(α, α), E=23.6-386.0 MeV; 209Bi(α, α), E=19.0-104 MeV; calculated σ(E, θ); deduced 4He microscopic optical model potential by Greens function method. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064618
2011HA28 Ann.Nucl.Energy 38, 1852 (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Calculation and evaluations for n + 63, 65, nat.Cu reactions NUCLEAR REACTIONS Cu, 63,65Cu(n, X), (n, n), (n, n'), (n, γ), (n, p), (n, d), (n, α), (n, 2n), (n, 3n), E<250 MeV; calculated σ, σ(θ). Optical model, preequilibrium theory, comparison with ENDF/B-VII.0, JENDL-3.3 evaluated nuclear libraries and experimental data.
doi: 10.1016/j.anucene.2011.05.016
2011HA29 Ann.Nucl.Energy 38, 1950 (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Double differential cross sections of n + 63, 65, nat.Cu reactions NUCLEAR REACTIONS Cu, 63,65Cu(n, X), (n, xn), (n, xp), (n, xα), (n, xd), (n, xt), E<200 MeV; calculated σ(θ, E). Optical model, unified Hauser-Feshbach and exciton model, comparison with ENDF/B-VII.0, JENDL-3.3 evaluated nuclear libraries and experimental data.
doi: 10.1016/j.anucene.2011.05.001
2011HA44 J.Korean Phys.Soc. 59, 855s (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen, C.Cai The Theoretical Calculation of Cross Section and Spectrum for n+238U Reaction up to 150 MeV NUCLEAR REACTIONS 238U(n, f), (n, xn), (n, d), (n, t), (n, p), (n, α), E=0-200 MeV; calculated σ, dσ(E, θ) using different reaction models.
doi: 10.3938/jkps.59.855
2011HA45 J.Korean Phys.Soc. 59, 859s (2011) Microscopic Optical Model Potential of Isospin Dependent Nucleon, Deuteron and Helium-3 NUCLEAR REACTIONS 58Ni(n, n), E=1.5-24.0 MeV;58Ni(p, p), E=7.0-20.0, 30.4, 35.2, 39.6, 61.4, 65.0 MeV;58Ni(d, d), E=4., 11.8-15.0, 28.6, 52.0, 56.0, 80.0, 120.0 MeV;58Ni(3He, 3He), E=21.9-43.7, 51.4, 73.2, 83.5, 89.3, 109.2, 118.5, 119.0 MeV; calculated σ(θ); deduced optical model parameters. 58Ni(p, X), E=5-100 MeV;58Ni(d, X), E=5-200 MeV;58Ni(3He, X), E=5-170 MeV; calculated σ; deduced optical model parameters. Microscopic optical model potential obtained using one-, two- and three-particle Green function method. Optical model parameters not stated in the paper.
doi: 10.3938/jkps.59.859
2011HA46 J.Korean Phys.Soc. 59, 1069s (2011) Present Status of Evaluated Nuclear Data Library for Accelerator-Driven Systems in China COMPILATION 24,25,26Mg, 27Al, 28,29,30Si, 40,42,43,44,46,48Ca, 50,52,53,54Cr, 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 90,91,92,94,96Zr, 93Nb, 91,94,95,96,97,98,100Mo, 180,182,183,184,186W, 204,206,207,208Pb, 209Bi, 232Th, 237Np, 232,233,234,235,236,237,238,239,240U, 236,244,245,245Pu, 241,242m,242,243Am, 243,244,245,246,247,248Cm(n, X), (p, X), E=0-200 MeV; calculated, evaluated σ, σ(E, θ).
doi: 10.3938/jkps.59.1069
2011LI05 Nucl.Instrum.Methods Phys.Res. B269, 597 (2011) Calculation and analysis of p + 40, 42, 43, 44, 46, 48, natCa reaction cross sections at incident energies from threshold to 250 MeV NUCLEAR REACTIONS 40,42,43,44,46,48Ca, Ca(p, p), (p, p'), (p, n), (p, 2n), (p, X), (p, 3He), (p, 2p), (p, xn), (p, xd), (p, x3He), (p, xα), E<250 MeV; calculated σ, σ(θ). Optical model calculations.
doi: 10.1016/j.nimb.2011.01.015
2011LI27 Nucl.Instrum.Methods Phys.Res. B269, 1899 (2011) Theoretical calculation and analysis of the p+59Co reaction NUCLEAR REACTIONS 59Co(p, X)57Co/58Co/56Co/56Mn/55Co/55Fe/54Mn/52Mn/51Cr, 59Co(p, n), (p, np), (p, 3n), (p, 4n), (p, xn), (p, xp), (p, xα), (p, xd), (p, xt), (p, x3He), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Optical model, comparison with experimental data.
doi: 10.1016/j.nimb.2011.05.014
2011ZH09 Nucl.Sci.Eng. 168, 151 (2011) Calculation and Analysis of Neutron-Induced Reactions on 59Co up to 200 MeV NUCLEAR REACTIONS 59Co(n, X), (n, n), (n, 2n), (n, 3n), (n, 4n), (n, 5n), (n, 4n2p), (n, xp), (n, xα), (n, xt), (n, xd), E<80 MeV; calculated σ, σ(θ), σ(E), σ(E, θ). Optical model, comparison with experimental data.
doi: 10.13182/NSE09-001
2010GU03 Phys.Rev. C 81, 044617 (2010) Deuteron microscopic optical model potential NUCLEAR REACTIONS 6Li, 9Be, 12C, 16O, 24Mg, 27Al, 28Si, 32S, 40Ar, 40,44,48Ca, 48Ti, 50,51V, 52Cr, 54,56Fe, 59Co, 58,60,64Ni, 63Cu, 68Zn, 70,72Ge, 89Y, 90Zr, 112,116,118,120,124Sn, 144,148,152Sm, 154,158,160Gd, 160,162,164Dy, 166,168,170Er, 172Yb, 180Hf, 186W, 208Pb(d, d), E=4-171 MeV; calculated σ, σ(E, θ) using nuclear matter approximation and local-density approximation based on Skyrme interaction; deduced deuteron microscopic optical model potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044617
2010HA06 Phys.Rev. C 81, 024616 (2010) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Global phenomenological optical model potential for nucleon-actinide reactions at energies up to 300 MeV NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np, 239,240,242Pu, 241Am(n, X), E=0.01-300 MeV; calculated total σ. 235,238U(n, n), E=0.01-300 MeV; calculated σ. 232Th, 235,238U, 239Pu(n, n'), E=0.1-300 MeV; calculated non-inelastic σ. 232Th, 235,238U, 239Pu(n, n), (n, n'), E=0.14-15.2 MeV; 238U(n, n), E=96 MeV; calculated σ(θ) for elastic σ, inelastic σ and elastic+inelastic σ. 232Th, 238U(p, X), E=0-300 MeV; calculated σ. 232Th, 235,238U(p, p), (p, p'), E=16-95 MeV; calculated σ(θ). global phenomenological optical model potential. Deduced of neutron and proton global optical model potential parameters. Comparison and analysis with experimental data.
doi: 10.1103/PhysRevC.81.024616
2010HA19 Nucl.Phys. A834, 495c (2010) Microscopic Optical Potential of Isospin Dependent Nucleon, Deuteron and Helium-3 Based on Skyrme Interactions NUCLEAR REACTIONS 56Fe(n, n), E=9.41, 9.97, 10.53, 11.00, 11.42, 11.98, 12.46, 13.07, 13.63, 14.09, 14.58, 21.6, 24.8, 26.0, 55.0, 65.0, 75.0 MeV; 56Fe(p, p), E=4.08, 5.02, 5.84, 6.56, 7.74, 10.93, 11.66, 16.0, 18.6, 19.1, 30.3, 39.8, 61.5, 65.0 MeV; 12C, 27Al, 58Ni, 59Co, 60,62,64Ni, 89Y, 90,92Zr(3He, 3He), E=119.0 MeV; 24Mg(d, d), E=56.0, 60.0, 60.6, 62.0, 64.0, 66.0, 68.0, 70.0, 72.0, 74.0, 76.0, 77.3, 78.0, 80.0, 90.0, 170.0 MeV; calculated σ(θ) using microscopic optical potential. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.075
2010SU15 Nucl.Instrum.Methods Phys.Res. B268, 2585 (2010) X.Su, H.Liang, Y.Han, C.Cai, Q.Shen The theoretical calculation of p+232Th reaction for energies up to 250 MeV NUCLEAR REACTIONS 232Th(p, n), (p, 2n), (p, 3n), (p, 6n), (p, xn), (p, xα), (p, xt), (p, F), (p, X), E<250 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Optical and Iwamoto-Harada models.
doi: 10.1016/j.nimb.2010.07.003
2009GU16 Phys.Rev. C 79, 064601 (2009) Helium-3 microscopic optical model potential based on the Skyrme interaction NUCLEAR REACTIONS 12C, 16O, 24Mg, 27Al, 28Si, 40Ca, 56Fe, 59Co, 58,60,62,64Ni, 63Cu, 89Y, 90,92Zr, 115In, 112,116,118,120,124Sn, 208Pb(3He, 3He), E<200 MeV; calculated microscopic optical potential, σ, σ(θ), rms radii, radial dependence, volume integral per nucleon using the Green function method and effective Skyrme interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064601
2009ZH02 Nucl.Sci.Eng. 161, 331 (2009) Theoretical Calculations and Analysis for the n + 59Co Reaction up to 20 MeV NUCLEAR REACTIONS 59Co(n, n), (n, n'), (n, γ), (n, p), (n, d), (n, α), (n, 2n), (n, X), E < 20 MeV; analyzed σ, σ(θ). Compared results to evaluated databases.
doi: 10.13182/NSE161-331
2006HA42 Phys.Rev. C 74, 044615 (2006) Deuteron global optical model potential for energies up to 200 MeV NUCLEAR REACTIONS 12C, 16O, 28Si, 40,48Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(d, X), E=0-200 MeV; calculated reaction σ. 12C, 16O, 24Mg, 27Al, 32S, 40Ar, 40,44,48Ca, 48,49Ti, 51V, 52Cr, 54Fe, 59Co, 58,62,64Ni, 63Cu, 64,68Zn, 89Y, 90,91,92,94,96Zr, 93Nb, 100Mo, 105Pd, 107Ag, 112Cd, 115In, 112,120,124Sn, 140Ce, 144,148,152Sm, 154,158,160Gd, 160,162,164Dy, 166,168,170Er, 172Yb, 180Hf, 181Ta, 186W, 197Au, 208Pb, 209Bi, 238U(d, d), E=4-200 MeV; calculated σ(θ). Global optical model parameters, comparison with data.
doi: 10.1103/PhysRevC.74.044615
2005HA12 Nucl.Sci.Eng. 150, 78 (2005) Calculations and Evaluations of Cross sections for n + 204, 206, 207, 208, natPb Reactions in the En ≤ 250 MeV Energy Range NUCLEAR REACTIONS Pb, 204,206,207,208Pb(n, X), (n, n), (n, n'), (n, γ), (n, xn), (n, F), E ≤ 250 MeV; compiled, analyzed σ.
doi: 10.13182/NSE05-A2503
2003HA40 Nucl.Sci.Eng. 143, 202 (2003) Y.Han, Q.Shen, J.Zhang, Z.Zhang Calculation and Analysis of n + 232Th Reaction Cross Sections NUCLEAR REACTIONS 232Th(n, X), (n, F), (n, γ), (n, n), (n, n'), (n, 2n), (n, nX), E=0.05-20 MeV; calculated, analyzed σ, σ(θ).
doi: 10.13182/NSE03-A2330
2003ZH41 Nucl.Sci.Eng. 143, 90 (2003) Z.Zhang, X.Sun, C.Cai, Q.Shen, Y.Han Calculations for Proton-Induced Reactions Below 250 MeV on 208Pb and 209Bi Targets NUCLEAR REACTIONS 208Pb, 209Bi(p, p), (p, X), E=10-400 MeV; analyzed elastic σ(θ), total σ; deduced optical model parameters. 209Bi(p, n), (p, 3n), (p, 4n), E<250 MeV; 208Pb(p, xn), (p, xnp), E < 250 MeV; 208Pb, 209Bi(p, nX), (p, pX), (p, dX), (p, tX), (p, αX), (p, 3HeX), E < 250 MeV; calculated σ. 208Pb(p, nX), E=11-45 MeV; 209Bi(p, nX), E=45-225 MeV; calculated neutron spectra. 208Pb(p, X)208Bi/207Bi/205Pb/204Pb/202Pb/204Tl/194Hg, E < 250 MeV; 209Bi(p, X)209Po/208Po/208Bi/207Bi/205Pb/204Pb/202Pb, E < 250 MeV; calculated production σ.
doi: 10.13182/NSE03-A2321
1997LI05 Nucl.Phys. A616, 131c (1997) W.Liu, X.Bai, S.Zhou, Z.Ma, Z.Li, Y.Wang, A.Li, Z.Ma, B.Chen, X.Tang, Y.Han, Q.Shen, J.Xu Measurement of the Angular Distribution for the 7Be(d, n)8B Reaction and Determination of the Astrophysical S Factor for the 7Be(p, γ)8B Reaction NUCLEAR REACTIONS, ICPND 7Be(d, n), E(cm)=5.8 MeV; measured σ(θ), reaction σ; deduced 7Be(p, γ) reaction astrophysical S-factor, model parameters.
doi: 10.1016/S0375-9474(97)00082-1
1996LI12 Phys.Rev.Lett. 77, 611 (1996) W.Liu, X.Bai, S.Zhou, Z.Ma, Z.Li, Y.Wang, A.Li, Z.Ma, B.Chen, X.Tang, Y.Han, Q.Shen Angular Distribution for the 7Be(d, n)8B Reaction at E(c.m.) = 5.8 MeV and the S17(0) Factor for the 7Be(p, γ)8B Reaction NUCLEAR REACTIONS, ICPND 2H(7Be, n), E(cm)=5.8 MeV; measured σ(θ); deduced astrophysical S-factor for 7Be(p, γ). DWBA analysis.
doi: 10.1103/PhysRevLett.77.611
1994SH11 Nucl.Sci.Eng. 117, 88 (1994) Nucleon Double-Differential Cross Section Based on Anisotropic Intranuclear Scattering NUCLEAR REACTIONS 1H(n, n), E=50-150 MeV; calculated σ(θ). 1H(n, n), E ≤ 100 MeV; calculed σ(E).
doi: 10.13182/NSE94-A20075
1994SH12 Nucl.Sci.Eng. 117, 99 (1994) Double-Differential Cross Section of Light Composite Particles in the Exciton Model NUCLEAR REACTIONS 56Fe(n, α), (n, d), E < 100 MeV; calculated σ(E). 56Fe(n, α), (n, d), E=14.8 MeV; 120Sn(p, α), (p, d), E=62 MeV; calculated σ(θ, Eα), σ(θ, Ed). 120Sn(p, t), E=62 MeV; calculated σ(θ, Et). Exciton model.
doi: 10.13182/NSE93-66
1994SH21 Phys.Rev. C50, 2473 (1994) Approach for Calculating Multistep Direct Reactions of Continuum and Discrete Levels NUCLEAR REACTIONS 11B(p, n), E=4-11 MeV; calculated σ(θ). 11B(p, n), E=3-20 MeV; 11B(p, X), (p, n), (p, p'), (p, nα), (p, α), (p, np), (p, d), (p, 3He), (p, t), (p, 2p), (p, 2n), E=1-25 MeV; calculated σ(E). Feshbach-Kerman-Koonin quantum multi-step direct reaction theory.
doi: 10.1103/PhysRevC.50.2473
1994SH30 Chin.J.Nucl.Phys. 16, No 2, 160 (1994) The Angular Distribution of Light Composite Particle Projectile in Preequilibrium Reactions NUCLEAR REACTIONS 56Fe(n, α), (n, d), E < 100 MeV; calculated ejectile first emission spectra. 120Sn(p, α), (p, d), E=62 MeV; calculated σ(θ, Eα), σ(θ, Ed). Preequilibrium theories.
1992SH20 Chin.J.Nucl.Phys. 14, No 3, 222 (1992) Analyses of Contributions of Direct Reaction and Preequilibrium Emission in E ≤ 50 MeV Energy Region NUCLEAR REACTIONS 56Fe(n, n'), (n, p), (n, α), (n, d), (n, np), (n, nα), E=5-50 MeV; calculated equilibrium, preequilibrium, direct emission relative σ; deduced model parameters. Optical, evaporation, exciton models.
1992SH28 Chin.J.Nucl.Phys. 14, No 4, 322 (1992) The Calculation of Excitation Functions for p + 89Y Reaction in E ≤ 40 MeV Energy Region with Microscopic Optical Potential NUCLEAR REACTIONS 89Y(p, n), (p, 2n), E ≤ 40 MeV; calculated σ(E). Many-body theory, microscopic optical potential, Skyrme forces.
1992ZH14 Chin.J.Nucl.Phys. 14, No 1, 7 (1992) Investigation of 89Y(p, n)89Zr, 89Y(p, 2n)88Zr and 89Y(p, pn)88Y Reactions up to 22 MeV NUCLEAR REACTIONS, ICPND 89Y(p, n), (p, 2n), (p, np), E=7-22 MeV; measured σ(E); deduced model parameters.
1992ZH29 Chin.J.Nucl.Phys. 14, No 3, 248 (1992) W.Zhao, Q.Shen, H.Lu, W.Yu, T.Liu Investigation of the Cross Sections for 89Zr(n, 2n)88Zr Reaction NUCLEAR REACTIONS 89Y(p, 2n), E=threshold-22 MeV; measured σ(E); deduced systematics calculation suitability for 89Zr(n, 2n) σ estimate. Activation method.
1991CA21 Nucl.Sci.Eng. 109, 142 (1991) Comparisons of Global Phenomenological and Microscopic Optical Potentials for Nuclear Data Predictions NUCLEAR REACTIONS 59Co(n, n), (n, n'), E ≤ 20 MeV; calculated σ(E). 59Co(n, n), E=2.47, 8 MeV; calculated σ(θ). 98Mo(n, p), (n, nα), (n, γ), (n, np), (n, α), E=threshold-20 MeV; 100Mo(n, 2n), E ≈ 8.5-20 MeV; calculated σ(E). Optical model from other data analysis.
doi: 10.13182/NSE91-A28513
1991CA26 Chin.J.Nucl.Phys. 13, No 1, 45 (1991) C.Cai, D.Liu, Q.Shen, Y.Tian, Y.Zhuo Comparison between Phenomenological and Microscopic Optical Potential in Nuclear Data Evaluations NUCLEAR REACTIONS 27Al, 31P, S, Cl, K, Ca, Fe, 59Co, Cu, Ag, In, Sb, W, Pb(n, n), E ≈ 0.083-24 MeV; calculated σ. Comparison with data. Different models chi square fits, phenomenological optimal, global and microscopic optical potentials.
1991LI27 Nucl.Phys. A534, 1 (1991) K.-F.Liu, H.Luo, Z.Ma, Q.Shen, S.A.Moszkowski Skyrme-Landau Parameterization on Effective Interactions (I). Hartree-Fock Ground States NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energy per nucleon, neutron, proton, charge radii. Skyrme-Landau effective interactions parametrization.
doi: 10.1016/0375-9474(91)90555-K
1991LI28 Nucl.Phys. A534, 25 (1991) Skyrme-Landau Parameterization of Effective Interactions (II). Self-Consistent Description of Giant Multipole Resonances NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated giant resonances, multipole transition strengths. Skyrme-Landau effective interactions parametrization.
doi: 10.1016/0375-9474(91)90556-L
1988TI04 Chin.J.Nucl.Phys. 10, 183 (1988) Tian Ye, Han Yinlu, Shen Qingbiao, Cai Chonghai Calculation and Analysis of Fast Neutron Cross Sections on Mo with Microscopic Optical Potential NUCLEAR REACTIONS 98Mo(n, p), (n, γ), (n, α), (n, np), 100Mo(n, 2n), E=threshold-20 MeV; calculated σ(E). 98Mo(n, n), E=0.5-26 MeV; calculated σ(θ). Hauser-Feshbach, preequilibrium exciton (with evaporation) models, microscopic optical potential.
1987YU02 Chin.J.Nucl.Phys. 9, 316 (1987) Yuan Haiji, Ye Weilei, Gao Qin, Shen Qingbiao, Zhuo Yizhong Microscopic Calculations of Single-Particle Spreading Width II. In Finite Nuclei NUCLEAR STRUCTURE 12C, 16O, 40Ca, 90Zr, 120Sn, 208Pb; calculated single particle spreading widths. Local density approximation.
1986SH37 Chin.J.Nucl.Phys. 8, 376 (1986) Empirical Formula of Nuclear Density fitting Experimental Data of Charge Radii and Charge Distributions NUCLEAR STRUCTURE A ≤ 208; calculated charge radii, distributions; deduced model parameters. Fermi type empirical formula.
1986TI05 Chin.J.Nucl.Phys. 8, 28 (1986) Tian Ye, Wang Chang, Han Yinlu, Shen Qingbiao, Zhuo Yizhong An Application of the Microscopic Optical Potential (S-MOP) to Non Even-Even Nuclei in Calculations of Cross Sections NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 14N, 23Na, 27Al, 51V, 53Cr, 55Mn, 59Co, 63,65Cu, 93Nb, 181Ta, 197Au, 235U, 239Pu(n, n), E ≈ 1-200 MeV; calculated total σ, σ(θ). Microscopic optical potential.
1986YE01 Chin.J.Nucl.Phys. 8, 15 (1986) Ye Weilei, Yuan Haiji, Gao Qin, Shen Qingbiao, Zhuo Yizhong The Calculations of Charge Density Distribution and Charge Radii for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces NUCLEAR STRUCTURE 48Ca, 90Zr; calculated levels. 16O, 40,48Ca, 90Zr; calculated charge density distributions. 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated charge rms radii. Hartree-Fock method.
1986YE02 Chin.J.Nucl.Phys. 8, 214 (1986) Ye Weilei, Yuan Haiji, Gao Qin, Zheng Chunkai, Tian Ye, Shen Qingbiao Calculations of Neutron Skin for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces NUCLEAR STRUCTURE 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated proton, neutron density distributions, rms radii. Hartree-Fock method, Skyrme force.
1985TI06 Chin.J.Nucl.Phys. 7, 207 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin Lifei A Global Analysis of Proton Differential Elastic Cross Section Calculations with the Microscopic Optical Potential S-MOP NUCLEAR REACTIONS 184W, 120Sn, 90Zr, 58,60,62,64Ni(p, p), E=16 MeV; 120Sn, 60Ni, 56Fe(p, p), E=30.3 MeV; 90Zr, 58Ni, 40Ca(p, p), E=40 MeV; 68Zn, 58Ni, 40Ca, 12C(p, p), E=61.4 MeV; 208Pb(p, p), E=16-61.4 MeV; analyzed σ(θ). Microscopic optical potential, extended Skyrme force.
1985TI07 Chin.J.Nucl.Phys. 7, 154 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei A Global Analysis of Integral Cross Section Calculations with the Microscopic Optical Potential NUCLEAR REACTIONS 12C(n, n), E ≤ 100 MeV; 44,40Ca(n, n), E ≤ 15 MeV; 60Ni(n, n), E ≤ 30 MeV; 242Pu, 98Mo(n, n), E ≤ 100 MeV; 140Ce(n, n), E ≤ 60 MeV; 238U, 232Th(n, n), E ≤ 15 MeV; calculated elastic, nonelastic, total σ(E). Effective Skyrme force, microscopic optical potential.
1985TI08 Chin.J.Nucl.Phys. 7, 344 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei A Global Analysis of Neutron Differential Elastic Cross Section Calculations with the Microscopic Optical Potential NUCLEAR REACTIONS 4He, 12C, 16O, 24Mg, 28Si, 32S, 40Ca, 50,52,54Cr, 54,56Fe, 58,60,62,64Ni, 64,66,68Zn, 90,92,94Zr, 92,94,96,98,100Mo, 118,120,122,124Sn, 182,184,186W, 208Pb, 232Th, 238U, 240Pu(n, n), E=1-26 MeV; calculated σ(θ). Microscopic optical potential.
1985YE02 Chin.J.Nucl.Phys. 7, 166 (1985) Ye Weilei, Yuan Haiji, Gao Qin, Shen Qingbiao, Zhang Jingshang, Liu Ruizhe, Gu Yingqi Hartree-Fock Calculations with Extended Skyrme Force for 16O and 40Ca NUCLEAR STRUCTURE 16O, 40Ca; calculated single particle energies. Hartree-Fock method, extended Skyrme force.
1985YU01 Chin.J.Nucl.Phys. 7, 332 (1985) Shell Model Calculations of 90Zr with Woods-Saxon Potential NUCLEAR STRUCTURE 90Zr; calculated levels, nucleon, spin, kinetic energy densities. Shell model.
1984SH37 Chin.J.Nucl.Phys. 6, 193 (1984) Shen Guanran, Huang Tangzi, Wen Shenlin, Yu Chunying, Li Anli, Tang Hongqing, Shen Qingbiao, Zhao Zhixiang, Gu Fuhua Fast Neutron Elastic Scattering Differential Cross Sections from 238U NUCLEAR REACTIONS 238U(n, n), E=14.2 MeV; measured σ(θ). Coupled-channels analysis. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30716. 1984SH38 Chin.J.Nucl.Phys. 6, 245 (1984) Shen Qingbiao, Tian Ye, Wang Shunuan, Gao Liangjun, Zhuo Yizhong, Zhao Fujian Exciton Transition Rate Calculations Based on the Optical Model Potentials NUCLEAR STRUCTURE 40Ca, 120Sn, 238U; calculated exciton transition rates. Optical potential, Skyrme interaction.
1982SH25 Chin.J.Nucl.Phys. 4, 24 (1982) Shen Qingbiao, Shi Xiangjun, Zhou Fuxiu Calculations of 115In(n, n')115mIn and Other Neutron Reaction Cross Sections NUCLEAR REACTIONS 115In(n, n), (n, γ), (n, n'), (n, X), E=0.1-9 MeV; calculated σ vs E. Optical model, Hauser-Feshbach formalism.
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