NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Guo Found 94 matches. 2024CH15 Chin.Phys.C 48, 014101 (2024) W.Chen, D.Pang, H.Guo, T.Ye, W.Sun, Y.Ying Elastic scattering and total reaction cross sections of 6Li examined via a microscopic continuum discretized coupled-channels model NUCLEAR REACTIONS 27Al, 64Zn, 138Ba, 208Pb(6Li, 6Li), (6Li, X) E<50 MeV; analyzed available data; deduced σ, σ(θ) at incident energies around the Coulomb barrier within the continuum discretized coupled-channels (CDCC) framework.
doi: 10.1088/1674-1137/ad0453
2023CH28 Phys.Rev. C 107, 064610 (2023) W.Chen, D.Y.Pang, H.Guo, Y.Tao, W.Sun, Y.J.Ying Continuum-discretized coupled-channels calculations for 6Li fusion reactions with closed channels NUCLEAR REACTIONS 28Si(6Li, X), E(cm)=4-20 MeV;64Ni(6Li, X), E(cm)=11-25 MeV;144Sm(6Li, X), E(cm)=19-37 MeV;209Bi(6Li, X), E=28-48 MeV; calculated total and complete fusion σ(E), partial-wave fusion σ for J up to 30. 2H(α, α), E(cm)<8 MeV; calculated scattering phase-shift. 6Li(e, e'), E not given; calculated charge form factors. Continuum-discretized coupled-channels method. Comparison to available experimental data.
doi: 10.1103/PhysRevC.107.064610
2023GU14 Appl.Radiat.Isot. 200, 110948 (2023), Erratum Appl.Radiat.Isot. 201, 111029 (2023) H.Guo, Q.Li, C.Zhang, L.Jiang, X.Ruan Measurement of the 134Xe(n, 2n)133m, gXe and 136Xe(n, 2n)135m, gXe reaction cross-sections and isomeric ratios induced by the 14.8 MeV neutrons NUCLEAR REACTIONS 134,136Xe(n, 2n), E=14.8 MeV; measured reaction products, Eγ, Iγ; deduced σ for ground and isomeric states. Comparison with available data. The 300 kV Cockcroft Walton Accelerator of China Institute of Atomic Energy.
doi: 10.1016/j.apradiso.2023.110948
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
2023ZH50 Chin.Phys.C 47, 114101 (2023) Ch.Zhu, H.Guo, J.Wang, P.Zheng, X.Lu, T.Zhu Measurement of 169Tm(n, 2n)168Tm reaction cross sections from 12 to 19.8 MeV NUCLEAR REACTIONS 169Tm, 93Nb(n, 2n), E=12-19.8 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, JENDL-4.0, JEFF=3.3 evaluated libraries. The 5SDH-2 1.7-MV Tandem accelerator in China.
doi: 10.1088/1674-1137/acf287
2022CH45 J.Phys.(London) G49, 075104 (2022) W.Chen, H.Guo, T.Ye, Y.-J.Ying, W.Sun, Y.Han Application of the Lagrange-mesh method in continuum-discretized coupled-channel calculations NUCLEAR REACTIONS 58Ni(d, X), E=80 MeV; 12C(6Li, X), E=168.6, 178 MeV; 59Co(6Li, X), E=12, 17.4, 18 MeV; analyzed available data; calculated the bound states and discretize the continuum states of weakly bound nuclei using the continuum-discretized coupled-channel (CDCC) method.
doi: 10.1088/1361-6471/ac7249
2022GU01 Nucl.Sci.Eng. 196, 40 (2022) H.Guo, W.Chen, Y.Han, X.Sun, T.Ye, W.Sun Theoretical Calculations and Evaluations of Neutron-Induced Reactions on 121Sb, 123Sb, and Natural Sb NUCLEAR REACTIONS 121,123Sb(n, X), Sb(n, n), (n, X), E<20 MeV; calculated σ, σ(θ). Comparison with CENDL-3, JENDL-4 libraries, experimental data.
doi: 10.1080/00295639.2021.1940067
2021GU15 Ann.Nucl.Energy 158, 108248 (2021) H.Guo, W.Chen, T.Ye, W.Sun, Y.Han, C.Cai Theoretical calculation of n+235U reaction NUCLEAR REACTIONS 235U(n, X)1NN/1H/2H/3H/3He/4He, E<150 MeV; calculated particle emission and γ-ray production σ, σ(θ), σ(θ, E). Comparison with ENDF/B-VIII.0 and JENDL-4.0 evaluated libraries.
doi: 10.1016/j.anucene.2021.108248
2021XU07 Chin.Phys.C 45, 114103 (2021) Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai Description of elastic scattering induced by the unstable nuclei 9, 10, 11, 13, 14C NUCLEAR REACTIONS 208Pb(9C, 9C), (11C, 11C), E=222-227 MeV; 27Al, 58Ni, 208Pb(10C, 10C), E=29.1-256 MeV; 28Si, 208Pb(9C, 9C), E<500 MeV; 28Si, 208Pb(11C, 11C), E<500 MeV; 28Si(13C, 13C), E=25-60 MeV; 40Ca, 56Fe, 60Ni, 66Zn, 88Sr(14C, 14C), E=51 MeV; 92,100Mo(14C, 14C), E=71 MeV; 28Si(14C, 14C), E<500 MeV; analyzed available data; deduced σ, σ(θ), global optical model potentials.
doi: 10.1088/1674-1137/ac1fe1
2020CH17 Chin.Phys.C 44, 054109 (2020) W.-D.Chen, H.-R.Guo, W.-L.Sun, T.Ye, Y.-J.Ying, Y.-L.Han, Q.B.Shen Microscopic study of 7Li-nucleus potential NUCLEAR REACTIONS 58Ni, 27Al, 65Cu, 89Y, 116Sn, 138Ba, 208Pb, 28Si, 13C(7Li, 7Li), E<300 MeV; analyzed available data. 7Li; calculated σ.
doi: 10.1088/1674-1137/44/5/054109
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
2020GU07 Ann.Nucl.Energy 142, 107363 (2020) H.Guo, W.Chen, T.Ye, W.Sun, Y.Han, C.Cai Theoretical calculation and evaluation of N + 237, 241, 243, 245Pu reactions NUCLEAR REACTIONS 237Pu(n, F), 241Pu(n, X), (n, γ), (n, F), Pu(n, X), (n, n'), (n, 2n), E<20 MeV; calculated σ using the optical model, distorted wave Born approximation theory, Hauser-Feshbach theory with width fluctuation correction, fission model, evaporation model, exciton model and the intranuclear cascade model. Comparison with ENDF/B-VIII, JENDL-4.0/HE and TENDL libraries.
doi: 10.1016/j.anucene.2020.107363
2020RE11 Phys.Rev. C 102, 034604 (2020) Z.Ren, Y.Yang, J.Wen, H.Guo, Z.Wen, R.Liu, Z.Han, W.Sun, X.Liu, Q.Chen, T.Ye, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the 236U(n, f) cross section for neutron energies from 0.4 MeV to 40 MeV from the back-streaming white neutron beam at the China Spallation Neutron Source NUCLEAR REACTIONS 235,236U(n, F), E AP 0.4-40 MeV beam from the China Spallation Neutron Source (CSNS)-Back-streaming white neutron source (WNS); measured fission fragments, energy spectra, time-of-flight using Fast Ionization Chamber Spectrometer; deduced 236U(n, F)/235U(n, F) cross section ratios. Comparison with theoretical calculation using the UNF code, and with evaluated data in JENDL-4.0, CENDL-3.1, and ENDF/B-VIII.0 libraries.
doi: 10.1103/PhysRevC.102.034604
2020XU03 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 12C, 27Al, 28Si, 58Ni, 208Pb(8B, 8B), 9Be, 12C, 16O, 28Si, 58Ni, 120Sn, 208Pb(10B, 10B), 12C, 28Si, 58Ni, 208Pb, 209Bi(11B, 11B), E<50 MeV; analyzed available data. 8,10,11B; calculated σ; deduced global phenomenological optical model potentials.
doi: 10.1088/1674-1137/44/3/034101
2020XU04 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 27Al, 58Ni, 208Pb, 12C, 28Si(8B, 8B), E<100 MeV; 27Al, 28Si, 58Ni, 120Sn, 16O, 9Be, 208Pb(10B, 10B), E<100 MeV; 28Si, 58Ni, 209Bi, 12C, 209Bi(11B, 11B), E<100 MeV; analyzed available data. 9Be; deduced optical model potential parameters, σ, σ(θ).
doi: 10.1088/1674-1137/44/3/034101
2020XU10 Chin.Phys.C 44, 124103 (2020) Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai Global optical model potential describing 12C-nucleus elastic scattering NUCLEAR REACTIONS 24Mg, 28Si, 32S, 39K, 40,42,48Ca, 50Cr, 56Fe, Fe, 58,64Ni, Ni, 90,91,92,94,96Zr, 92Mo, 116,117,118,119,120,122,124Sn, 194,198Pt, 208Pb, 209Bi(12C, 12C), E<200 MeV; analyzed available data; deduced a new global optical model potential parameters.
doi: 10.1088/1674-1137/abb4d0
2020ZH26 Chin.Phys.C 44, 094001 (2020) J.Zhong, Y.-J.Ma, X.-G.Wu, B.-J.Zhu, C.-B.Li, G.-S.Li, Y.Zheng, Q.-M.Chen, C.-Y.He, L.-T.Deng, W.-K.Zhou, K.-Y.Ma, D.Yang, H.Guo, J.-Q.Wang, X.Guang, J.Sun, H.-B.Sun, S.-P.Hu, L.Gan, H.-G.Zhao, Q.Luo, Z.-X.Wu Lifetime measurement for the 21+ state in 106Cd NUCLEAR REACTIONS 94Zr(16O, 4n)106Cd, E=87 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, lifetime, B(E2). The Recoil Distance Doppler Shift technique in combination with the Differential Decay Curve Method.
doi: 10.1088/1674-1137/44/9/094001
2019GU07 Phys.Rev. C 99, 034602 (2019) H.Guo, Y.Watanabe, T.Matsumoto, K.Nagaoka, K.Ogata, M.Yahiro Analysis of nucleon and triton emissions from nucleon-7Li collisions below 20 MeV NUCLEAR REACTIONS 7Li(n, n), (n, n'), E=4.08, 5.1, 6.1, 6.97, 7.97, 9, 10, 11, 12, 13, 14, 15.4, 18 MeV; calculated σ(θ, E) and compared with experimental data. 7Li(p, t), E=14 MeV; 7Li(n, t), E=11.5, 14, 14.2, 18 MeV; calculated t-α scattering phase shifts, double-differential σ(E, θ) of break-up and reaction channels, and integrated neutron induced σ using continuum discretized coupled-channels (CDCC) method, final-state interaction model, and sequential decay model. Comparison with experimental and evaluated data.
doi: 10.1103/PhysRevC.99.034602
2019XU05 Phys.Rev. C 99, 034618 (2019) Y.Xu, Y.Han, H.Liang, Z.Wu, H.Guo, C.Cai Global optical model potential for the weakly bound projectile 9Be NUCLEAR REACTIONS Mg(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 27Al(9Be, 9Be), E=12.0, 14.0, 18.0, 20.0, 22.0, 25.0, 28.0, 32.0, 33.0, 35.0.40.0, 47.5 MeV; 28Si(9Be, 9Be), E=12.0, 13.0, 14.0, 17.0, 20.0, 23.0, 26.0, 30.0, 45.0, 50.0, 60.0 MeV; 40Ca(9Be, 9Be), E=14.0, 20.0, 26.0, 45.0.50.0, 60.0 MeV; 58Ni(9Be, 9Be), E=20.0, 26.0 MeV; 64Zn(9Be, 9Be), E=17.0, 19.0, 21.0, 23.0, 26.0, 28.0, 28.4, 28.97 MeV; 89Y(9Be, 9Be), E=18.6, 20.6, 22.7, 24.7, 26.7, 28.7, 33.2 MeV; Ag(9Be, 9Be), E=26.0 MeV; 144Sm(9Be, 9Be), E=30.0, 31.5, 33.0, 34.0, 35.0, 37.0, 39.0, 41.0, 44.0, 48.0 MeV; 208Pb(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 9.5, 40.0, 41.0, 42.0, 44.0, 46.0, 47.2, 48.0, 50.0, 60.0, 68.0, 75.0 MeV; 209Bi(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 39.5, 40.0, 41.0, 42.0, 44.0, 46.0, 48.0 MeV; analyzed elastic σ(θ, E) data for global phenomenological energy-dependent optical model potential parameters for 9Be. 9Be, 12,13C, 27Al, 64Zn, 89Y, 144Sm(9Be, X), E=10-300 MeV; 28Si, Cu(9Be, X), E=10-500 MeV; 89Y(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (9Be, X), (11B, X); calculated reaction σ(E) using optical model and compared with experimental data. 9Be(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 12C(9Be, 9Be), E=13.0, 14.0, 14.5, 17.3, 19.0, 20.0, 21.0, 26.0, 153.8 MeV; 13C(9Be, 9Be), E=19.46, 25.05 MeV; 16O(9Be, 9Be), E=20.0, 25.94 MeV; calculated elastic σ(θ, E) using optical model parameters and compared with experimental data.
doi: 10.1103/PhysRevC.99.034618
2018GU18 Chin.Phys.C 42, 124101 (2018) Double differential cross sections of light charged particle production for the n+238U reaction NUCLEAR REACTIONS 238U(n, X)1H/2H/3H/4He, E<150 MeV; calculated fission σ, ←E). Comparison with ENDF/B-VII, JENDL-4. evaluated libraries.
doi: 10.1088/1674-1137/42/12/124101
2018XU01 Phys.Rev. C 97, 014615 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai Global phenomenological optical model potential for the 7Li projectile nucleus NUCLEAR REACTIONS 9Be(7Li, 7Li), E=15.75, 24.0, 30.0, 63.0, 130.0 MeV; 12C(7Li, 7Li), E=7.5, 9.0, 12.0, 15.0, 36.0, 131.8 MeV; 16O(7Li, 7Li), E=26.0, 36.0, 42.0, 50.0 MeV; 11B, 12,13C, 24Mg(7Li, 7Li), E=34.0 MeV; 24,26Mg(7Li, 7Li), E=88.7 MeV; 27Al(7Li, 7Li), E=6.0, 7.0, 8.0, 9.0, 10.0, 11.0, 12.0, 13.0, 14.0, 16.0, 18.0, 19.0, 24.0 MeV; 28Si(7Li, 7Li), E=8.0, 8.5, 9.0, 10.0, 11.0, 11.5, 13.0, 15.0, 16.0, 21.0, 26.0, 36.0, 177.8 MeV; 40,44,48Ca(7Li, 7Li), E=34.0; 40Ca(7Li, 7Li), E=88.7 MeV; 46,48Ti(7Li, 7Li), E=17.0 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe, 65Cu, 90Zr(7Li, 7Li), E=34.0 MeV; 58Ni(7Li, 7Li), E=14.22, 16.25.18.28, 19.0, 20.31.34.0, 42.0 MeV; 60,62Ni, 64,68Zn(7Li, 7Li), E=34.0 MeV; 80Se(7Li, 7Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 23.0, 26.0 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 116Sn(7Li, 7Li), E=18.0, 19.0, 20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0 MeV; 120Sn(7Li, 7Li), E=19.5, 20.0, 20.5, 22.0, 24.0, 25.0, 26.0, 28.0, 30.044.0 MeV; 138Ba(7Li, 7Li), E=21.0, 22.0, 23.0, 24.0, 28.0, 30.0, 32.0, 52.0 MeV; 140Ce, 142Nd(7Li, 7Li), E=52.0 MeV; 144Sm(7Li, 7Li), E=21.6, 22.1, 22.6.23.0, 25.0, 27.0, 29.0, 30.0, 32.0, 35.0, 40.8, 52.0 MeV; 208Pb(7Li, 7Li), E=27.0, 29.0, 33.0, 39.0, 42.0, 52.0 MeV; 232Th(7Li, 7Li), E=24.0, 26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed σ(θ, E) experimental data by global phenomenological optical model potential. 13C, 27Al, 64Zn, 116Sn, 138Ba, (7Li, X), E<300 MeV; 28Si, Cu, 208Pb(7Li, X), E<400 MeV; calculated reaction σ(E) using optical model, and compared with experimental data.
doi: 10.1103/PhysRevC.97.014615
2018XU10 Phys.Rev. C 98, 024619 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai 6Li global phenomenological optical model potential NUCLEAR REACTIONS 24Mg, 48Ca(6Li, 6Li), E=240.0 MeV; 25,26Mg, 39K, 91Zr(6Li, 6Li), E=34.0 MeV; 27Al(6Li, 6Li), E=7.0, 8.0, 10.0, 12.0, 18.0, 34.0 MeV; 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 16.0, 20.0, 21.0, 25.0, 27.0, 34.0, 46.0, 99.0, 135.0, 154.0, 210.0, 240.0, 318.0, 350.0 MeV; 40Ca(6Li, 6Li), E=50.6, 99.0, 156.0, 210.0, 240.0 MeV; 54Fe(6Li, 6Li), E=38.0, 44.0, 50.0 MeV; 59Co(6Li, 6Li), E=12.0, 18.0, 26.0, 30.0 MeV; 58Ni(6Li, 6Li), E=9.85, 11.21, 12.13, 13.04, 14.04, 34.0, 50.6, 73.7, 90.0, 99.0, 210.0, 240.0 MeV; 65Cu(6Li, 6Li), E=25.0 MeV; 64Zn(6Li, 6Li), E=10.77, 11.69, 12.0, 12.43, 13.0, 13.54, 13.8, 14.92, 15.0, 16.30, 16.5, 18.0, 18.14, 19.98, 22.0 MeV; 72,74,76Ge(6Li, 6Li), E=28.0 MeV; 80Se(6Li, 6Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 22.19, 23.0, 26.0 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=11.0, 12.0, 13.0, 15.0, 17.0, 19.0, 21.0, 25.0, 30.0, 34.0, 60.0, 70.0, 73.7, 99.0, 156.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 112Sn(6Li, 6Li), E=21.0, 22.0, 23.0, 25.0, 30.0, 35.0 MeV; 116Sn(6Li, 6Li), E=20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0, 40.0 MeV; 118Sn(6Li, 6Li), E=42.0 MeV; 120Sn(6Li, 6Li), E=30.0, 44.0, 90.0 MeV; 124Sn(6Li, 6Li), E=73.7 MeV; 138Ba(6Li, 6Li), E=21.0, 22.0, 23.0, 24.0, 26.0, 28.0 MeV; 144Sm(6Li, 6Li), E=21.0, 22.1, 22.6, 24.1, 26.0, 28.0, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25.0, 29.0, 31.0, 33.0, 35.0, 36.0, 37.0, 39.0, 42.0, 43.0, 46.0, 48.0, 50.6, 73.7, 88.0, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=24.0, 26.0, 28.0, 29.9, 30.0, 32.0, 32.8, 34.0, 36.0, 40.0, 44.0, 50.0 MeV; 232Th(6Li, 6Li), E=26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed differential σ(θ, E) data; deduced a new set of 6Li global phenomenological energy-dependent optical potential parameters based on the form of the Woods-Saxon potential within the optical model. 63,65Cu, 64Zn, 112,116Sn, 138Ba, 208Pb(6Li, X), E<400 MeV; calculated reaction σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.98.024619
2018XU12 Int.J.Mod.Phys. E27, 1850099 (2018) Y.-Li.Xu, H.-R.Guo, Y.-L.Han, Q.-B.Shen Global phenomenological optical model potentials for 8, 10, 11B projectiles NUCLEAR REACTIONS 28,30Si, 40Ca, 58Ni, 208Pb, 209Bi(11B, 11B), E<100 MeV; 7Li, 9Be, 12C, 28Si, 58Ni, 208Pb(8B, 8B), E < 100 MeV; 16O, 28Si, 120Sn, 208Pb, 232Th(10B, 10B), E<100 MeV; analyzed available data for 11B; deduced global phenomenological optical model potential for 11B, calculated σ.
doi: 10.1142/S0218301318500994
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
2017GU15 Ann.Nucl.Energy 108, 151 (2017) H.Guo, Y.Han, T.Ye, W.Sun, C.Cai Theoretical analysis and evaluation for neutron-induced reaction on 239Pu NUCLEAR REACTIONS 239Pu(n, X), (n, n), (n, n'), E<200 MeV; calculated σ, σ(θ, E). Comparison with ENDF/B-VII, JENDL-4 libraries, experimental data.
doi: 10.1016/j.anucene.2017.04.043
2017SU16 Phys.Rev. C 95, 054606 (2017) X.W.Su, Y.L.Han, H.Y.Liang, Z.D.Wu, H.R.Guo, C.H.Cai Global phenomenological optical model potential for 8Li projectile NUCLEAR REACTIONS 9Be(8Li, 8Li), E=14, 19.6, 27 MeV; 12C(8Li, 8Li), E=14, 23.9 MeV; 13C, 14N, 27Al, 197Au(8Li, 8Li), E=14 MeV; 51V(8Li, 8Li), E=18.5, 26 MeV; 58Ni(8Li, 8Li), E=14, 19.6, 20.2, 22 MeV; 208Pb(8Li, 8Li), E=24.4, 27.9, 28.9, 30.6, 33.1 MeV; calculated σ(θ, E) by optical potential model, and compared with experimental data; deduced global phenomenological optical model parameters (OMPs) for 8Li. 9Be(8Li, X), E=19.6 MeV; 12C(8Li, X), E=14 MeV; 51V(8Li, X), E=18.5, 26.0 MeV; 208Pb(8Li, X), E=24.4, 27.6, 28.89, 30.57, 33.13 MeV; calculated total σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.95.054606
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
2016SU13 Int.J.Mod.Phys. E25, 1650033 (2016) X.-W.Su, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Global 6He optical model potential NUCLEAR REACTIONS 6,7Li, 9Be, 12C, 27Al, 28Si, 51V, 48Ti, 58Ni, 63,65Cu, 64Zn, 120Sn, 197Au, 206,208Pb, 209Bi(6He, X), (6He, 6He), E<300 MeV; analyzed available data; deduced optical potential; calculated σ, σ(θ).
doi: 10.1142/S0218301316500336
2016SU14 Phys.Rev. C 93, 064301 (2016) J.Sun, Y.-J.Ma, T.Komatsubara, K.Furuno, Y.-H.Zhang, W.-P.Zhou, S.-Y.Wang, X.-Y.Hu, H.Guo, J.-Q.Wang, Y.-Z.Liu Bandhead energies in 125Cs NUCLEAR REACTIONS 116Cd(14N, 5n), E=65 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO) using Nordball array at NBI facility. 125Cs; deduced high-spin levels, J, π, multipolarity, bands, configurations; revised bandhead energies of the h11/21/2[550] and g9/29/2[404] configurations. Systematics of low-lying positive-parity g7/2 and d5/2 bands and staggering in 125,127,129Cs.
doi: 10.1103/PhysRevC.93.064301
2016SU26 Chin.Phys.C 40, 124001 (2016) J.Sun, T.Komatsubara, J.-Q.Wang, Ha.Guo, X.-Y.Hu, Y.-J.Ma, Y.-Z.Liu, K.Furuno Evidence for coexisting prolate and near-oblate shapes at high spin in 125Cs NUCLEAR REACTIONS 116Cd(14N, 5n), E=65 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, near oblate band at high spins. Comparison the geometrical model, cranked shell model and total Routhian surfaces model calculations.
doi: 10.1088/1674-1137/40/12/124001
2016XU02 Int.J.Mod.Phys. E25, 1650013 (2016) Y.-L.Xu, H.-R.Guo, Y.-L.Han, Q.-B.Shen The neutron microscopic optical potential based on skyrme interaction NUCLEAR REACTIONS 24Mg, 54,56Fe, 59Co, 90Zr, 93Nb, 92,96,98,100Mo, 120Sn, 206,208Pb(n, n), E=11 MeV; 12C, 16O, 23Na, 14N, 232Th, 235,238U, 239Pu(n, X), E=0.1-100 MeV; calculated σ(θ), σ. Comparison with experimental data.
doi: 10.1142/S0218301316500130
2015XU04 Int.J.Mod.Phys. E24, 1550005 (2015) Y.-L.Xu, H.-R.Guo, Y.-L.Han, Q.-B.Shen Applicability of the systematic helium-3 potential for triton-nucleus reactions NUCLEAR REACTIONS 28Si, 58Ni, 116Sn, 208Pb(t, t), (3He, 3He), E<60 MeV/nucleon; calculated σ; deduced optical model potential parameters. Comparison with available data.
doi: 10.1142/S0218301315500056
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
2014GU12 Nucl.Data Sheets 118, 254 (2014) H.Guo, K.Nagaoka, Y.Watanabe, T.Matsumoto, K.Ogata, M.Yahiro Application of the Continuum Discretized Coupled Channels Method to Nucleon-induced Reactions on 6, 7Li for Energies up to 150 MeV NUCLEAR REACTIONS 6Li(p, x), E=5-150 MeV; calculated reaction σ. 6Li(n, n'), E=14.1 MeV;7Li(p, p'), E=5-50 MeV;7Li(p, p'), (p, t), E=14 MeV; calculated σ(Eout, θ). CDCC with folding of complex JLM effective nucleon-nucleon forces. Compared with available data.
doi: 10.1016/j.nds.2014.04.051
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
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
2013GU06 Phys.Rev. C 87, 024610 (2013) H.Guo, Y.Watanabe, T.Matsumoto, K.Ogata, M.Yahiro Systematic analysis of nucleon scattering from 6, 7Li with the continuum discretized coupled channels method NUCLEAR REACTIONS 6,7Li(n, n), (n, n'), (p, p), (p, p'), E=0-150 MeV; analyzed total σ(E), reaction σ(E), σ(θ, E). Continuum discretized coupled channels method (CDCC).
doi: 10.1103/PhysRevC.87.024610
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
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
2011ZH26 Nucl.Sci.Eng. 169, 188 (2011) C.Zhu, Y.Chen, Y.Mou, P.Zheng, T.He, X.Wang, L.An, H.Guo Measurements of (n, 2n) Reaction Cross Sections at 14 MeV for Several Nuclei NUCLEAR REACTIONS 85,87Rb, 89Y, 140,142Ce, 169Tm, 175Lu, 181Ta, 185Re, 238U(n, 2n), E=14 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VII.0 evaluated nuclear data library.
doi: 10.13182/NSE10-35
2010GU01 Chin.Phys.Lett. 27, 012401 (2010) A Microscopic Optical Potential for Deuteron NUCLEAR REACTIONS 40Ca(d, X), (d, d), (d, d'), E=10-110 MeV; calculated microscopic optical potential for deuteron; deduced σ, σ(θ). Comparison with experimental data.
doi: 10.1088/0256-307X/27/1/012401
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
2009DO23 Chin.Phys.C 33, Supplement 1, 58 (2009) B.-G.Dong, H.-C.Guo, H.-L.Ma, Y.-L.Yan Description of all observed rotational bands in 128Pr NUCLEAR STRUCTURE 128Pr; calculated neutron and proton configurations, deformation, rotational bands. Configuration-dependent cranked Nilsson-Strutinsky (CNS) approach.
doi: 10.1088/1674-1137/33/S1/019
2009GU05 Nucl.Phys. A823, 83 (2009) Relativistic BCS-BEC crossover of a two-species Fermi gas with number density asymmetry at zero temperature
doi: 10.1016/j.nuclphysa.2009.03.003
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
2009SH31 Phys.Rev. C 80, 024604 (2009) Isospin dependent nucleon-nucleus optical potential with Skyrme interactions NUCLEAR REACTIONS 27Al, 56Fe, 208Pb(n, n'), (n, X), (p, p'), E<100 MeV; calculated σ. 27Al(n, n), E=1.5-96.0 MeV; 27Al(p, p), E=2.004-95.7 MeV; 56Fe(n, n), E=9.41-75.0 MeV; 56Fe(p, p), E=4.08-65.0 MeV; 208Pb(n, n), E=1.8-65.0 MeV; 208Pb(p, p), E=16.0-80 MeV; calculated σ(θ). 56Fe(n, X), (p, X), E=10-90 MeV; calculated radial dependence of neutron and proton microscopic optical potential (MOP). 27Al, 56Fe, 90Zr, 127I, 169Tm, 208Pb(p, X), E<120; calculated isospin effect values. Isospin dependent nucleon-nucleus optical potential calculations with Skyrme interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024604
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
2008HA15 Nucl.Instrum.Methods Phys.Res. B266, 1943 (2008) Light charged particle emission for p+54, 56, 57, 58, natFe reactions NUCLEAR REACTIONS 54,56,57Fe(p, X), Fe(p, x) E=25-200 MeV; calculated energy spectra and production cross sections of light charged particles; Compared results with theoretical models and existing experimental data.
doi: 10.1016/j.nimb.2008.03.188
2008HA33 Ann.Nucl.Energy 35, 2031 (2008) Double differential cross sections of neutron and proton emission in neutron induced reactions on 54, 56, 57, 58Fe NUCLEAR REACTIONS 56Fe(n, X), (n, pX), (n, nX), E < 200 MeV; 54,57,58Fe(n, pX), E < 200 MeV; calculated σ(θ, E). Compared results to available data.
doi: 10.1016/j.anucene.2008.06.002
2008HA38 Nucl.Sci.Eng. 161, 90 (2008) Calculation and Evaluations for n + 54, 56, 57, 58, natFe Reactions NUCLEAR REACTIONS 54,56,57,58Fe, Fe(n, X), E < 200 MeV; calculated and analyzed S(θ). Compared results to evaluated databases.
doi: 10.13182/NSE161-90
2007CH24 Phys.Rev. C 75, 035806 (2007) Neutrino scattering rates in neutron star matter with Δ isobars
doi: 10.1103/PhysRevC.75.035806
2007HA52 Nucl.Instrum.Methods Phys.Res. B265, 461 (2007) Calculation and evaluation of cross-sections for p+54, 56, 57, 58, natFe reactions up to 250 MeV NUCLEAR REACTIONS Fe(p, x)51Cr, E=0-200 MeV; Fe(p, x)55Co, E=13-80 MeV; Fe(p, x)54Mn, E=0-200 MeV; Fe(p, x)56Co, E=5-100 MeV; 58Fe(p, 3n2p)54Mn, E=15-60 MeV; 58Fe(p, 2n)57Co, E=12-40 MeV; 58Fe(p, 3n)56Co, E=24-60 MeV; 58Fe(p, n)58Co, E=3-40 MeV; 57Fe(p, 2p)58Mn, E=16-100 MeV; 57Fe(p, n)57Co, E=1-40 MeV; 57Fe(p, 2n)56Co, E=13-50 MeV; 58Fe(p, n2p)54Mn, E=20-100 MeV; 56Fe(p, 3n2p)52Mn, E=19-50 MeV; 56Fe(p, 2n)55Co, E=16-50 MeV; 56Fe(p, np)55Fe, E=13-50 MeV; 56Fe(p, n)56Co, E=1-50 MeV; 54Fe(p, 2n2p)54Mn, E=9-40 MeV; 56Fe(p, p'), E=6.0-61.5 MeV; 54Fe(p, p'), E=65 MeV; 54Fe(p, p), E=3.73-65.0 MeV; 56Fe(p, p), E=4.08-182.4 MeV; 56Fe(p, p'), E=6.0-61.5 MeV; 54,56Fe(p, p'), E=0-200 MeV; calculated cross sections, angular distributions, optical model, intra-nuclear cascade model, energy spectra of n, p, d, t, He and α-particle emission. Comparisons with nuclear model calculations and experimental data.
doi: 10.1016/j.nimb.2007.09.048
2006DO13 Phys.Rev. C 74, 014308 (2006) B.-G.Dong, H.-C.Guo, I.Ragnarsson Triaxial shape induced by couplings between equatorial orbitals NUCLEAR STRUCTURE 126,128,130,132Pr; calculated rotational bands energies, signature splitting, triaxial deformation. Configuration-dependent cranking calculations.
doi: 10.1103/PhysRevC.74.014308
2006GU13 Phys.Rev. C 73, 055803 (2006) J.Gu, H.Guo, X.Li, Y.Liu, F.Xu Antikaon condensation and deconfinement phase transition in neutron stars
doi: 10.1103/PhysRevC.73.055803
2006GU27 Eur.Phys.J. A 30, 455 (2006) J.F.Gu, H.Guo, X.G.Li, Y.X.Liu, F.R.Xu Phase transition to color-flavor-locked matter and condensation of Goldstone bosons in neutron star matter
doi: 10.1140/epja/i2006-10142-5
2005CH23 Nucl.Phys. A750, 324 (2005) Density dependence of nucleon radius and mass in the global color symmetry model of QCD with a sophisticated effective gluon propagator
doi: 10.1016/j.nuclphysa.2005.01.020
2005CH35 Eur.Phys.J. A 24, 211 (2005) Quasielastic electron scattering in relativistic mean-field theory NUCLEAR REACTIONS 40,48Ca, 56Fe, 208Pb(e, e'), E not given; calculated longitudinal response functions, Coulomb sum rule for quasielastic scattering. Density-dependent relativistic hadron field theory, comparison with data.
doi: 10.1140/epja/i2004-10141-6
2005CH72 Phys.Rev. D 72, 094023 (2005) Pion-nucleon sigma term in the global color model of QCD
doi: 10.1103/PhysRevD.72.094023
2005LI07 Chin.Phys.Lett. 22, 298 (2005) Lambda Hypernuclei in a Chiral Hadronic Model NUCLEAR STRUCTURE 16O, 28Si, 40Ca, 51V, 89Y, 208Pb; calculated hyperon binding energies. 16O, 40Ca, 208Pb; calculated hypernucleus binding energies, radii, spin-orbit splitting.
doi: 10.1088/0256-307X/22/2/009
2005LI37 Eur.Phys.J. A 25, 293 (2005) B.Liu, H.Guo, M.Di Toro, V.Greco Neutron stars with isovector scalar correlations
doi: 10.1140/epja/i2005-10095-1
2004DO15 Chin.Phys.Lett. 21, 2144 (2004) Band Structure in the Doubly Magic Nucleus 56Ni NUCLEAR STRUCTURE 56Ni; calculated rotational bands energies, moments of inertia, transition quadrupole moments, band termination features. Configuration-dependent cranked Nilsson-Strutinsky approach, comparison with data.
doi: 10.1088/0256-307X/21/11/019
2004GU08 Chin.Phys.Lett. 21, 817 (2004) H.Guo, R.Zhou, Y.-X.Liu, B.Liu, X.-G.Li In-Medium K+ and K- Production and K- Condensation in Supernova Matter
doi: 10.1088/0256-307X/21/5/015
2004LI67 Eur.Phys.J. A 22, 337 (2004) B.Liu, H.Guo, V.Greco, U.Lombardo, M.Di Toro, C.-D.Lu Equation of state of nuclear matter and neutron stars in a hadron mass scaling frame
doi: 10.1140/epja/i2003-10235-7
2004SA56 Phys.Rev. C 70, 044613 (2004) P.K.Saha, H.Noumi, D.Abe, S.Ajimura, K.Aoki, H.C.Bhang, K.Dobashi, T.Endo, Y.Fujii, T.Fukuda, H.C.Guo, O.Hashimoto, H.Hotchi, K.Imai, E.H.Kim, J.H.Kim, T.Kishimoto, A.Krutenkova, K.Maeda, T.Nagae, M.Nakamura, H.Outa, T.Saito, A.Sakaguchi, Y.Sato, R.Sawafta, M.Sekimoto, Y.Shimizu, T.Takahashi, H.Tamura, L.Tang, K.Tanida, T.Watanabe, H.H.Xia, S.H.Zhou, X.F.Zhu, L.H.Zhu Σ-nucleus potential studied with the (π-, K+) reaction on medium-to-heavy nuclear targets NUCLEAR REACTIONS H, C, Si, Ni, In, Bi(π-, K+X), E at 630-780 MeV/c; measured particle spectra, angular distributions; deduced Σ hyperon binding energies, Σ-nucleus potential features.
doi: 10.1103/PhysRevC.70.044613
2003DO03 Eur.Phys.J. A 17, 25 (2003) Band termination in the Z=N odd-odd nuclei 46V and 50Mn NUCLEAR STRUCTURE 46V, 50Mn; calculated rotational band energies, deformation, band termination features. Configuration-dependent cranked mean-field.
doi: 10.1140/epja/i2002-10142-5
2003GU04 Phys.Rev. C 67, 024902 (2003) Antikaon condensation and in-medium (anti)kaon production in β equilibrium nuclear matter
doi: 10.1103/PhysRevC.67.024902
2003GU14 Phys.Rev. C 68, 035803 (2003) H.Guo, Y.Chen, B.Liu, Q.Zhao, Y.Liu Effects of neutrino trapping on K and K-bar production and K-bar condensation in supernova matter
doi: 10.1103/PhysRevC.68.035803
2003LI36 Nucl.Phys. A725, 127 (2003) Y.-X.Liu, D.-F.Gao, J.-H.Zhou, H.Guo Reevaluation of the density dependence of nucleon radius and mass in the global color symmetry model of QCD NUCLEAR STRUCTURE 1n, 1H; calculated radius vs density in nuclear matter. Color symmetry model.
doi: 10.1016/S0375-9474(03)01574-4
2003LI39 Phys.Rev. C 68, 035204 (2003) Quark condensates in nuclear matter in the global color symmetry model of QCD
doi: 10.1103/PhysRevC.68.035204
2002GU23 Chin.Phys.Lett. 19, 1432 (2002) Proton Fraction in Hot Neutron Star Matter with a Chiral Hadronic Model
doi: 10.1088/0256-307X/19/10/311
2002NO09 Phys.Rev.Lett. 89, 072301 (2002); Erratum Phys.Rev.Lett. 90, 049902 (2003) H.Noumi, P.K.Saha, D.Abe, S.Ajimura, K.Aoki, H.C.Bhang, T.Endo, Y.Fujii, T.Fukuda, H.C.Guo, K.Imai, O.Hashimoto, H.Hotchi, E.H.Kim, J.H.Kim, T.Kishimoto, A.Krutenkova, K.Maeda, T.Nagae, M.Nakamura, H.Outa, M.Sekimoto, T.Saito, A.Sakaguchi, Y.Sato, R.Sawafta, Y.Shimizu, T.Takahashi, L.Tang, H.Tamura, K.Tanida, T.Watanabe, H.H.Xia, S.H.Zhou, L.H.Zhu, X.F.Zhu Sigma-Nucleus Potential in A = 28 NUCLEAR REACTIONS Si(π-, K+), E at 1.2 GeV/c; measured missing mass, σ(E, θ); deduced Σ-nucleus potential features.
doi: 10.1103/PhysRevLett.89.072301
2002WA11 Nucl.Phys. A705, 455 (2002) P.Wang, H.Guo, Z.Y.Zhang, Y.W.Yu, R.K.Su, H.Q.Song Multi-Strange Hadronic Systems in Chiral SU(3) Quark Mean Field Model NUCLEAR STRUCTURE 16O, 208Pb; calculated charge densities, single-proton energy levels. 4,5,6He, 7,8,9Li, 7,8,9,10Be, 9,10,11,12B, 15N, 40Ca, 51V, 89Y, 208Pb; calculated hypernucleus binding energies. 6He, 10Be, 13B; calculated double-Λ hypernucleus binding energies. Other multi-strange and purely hyperonic nuclides discussed. Chiral SU(3) quark mean field model.
doi: 10.1016/S0375-9474(02)00676-0
2002WA15 J.Phys.(London) G28, 2265 (2002) P.Wang, H.Guo, Y.B.Dong, Z.Y.Zhang, Y.W.Yu Chiral Symmetry Restoration of Nuclear Matter
doi: 10.1088/0954-3899/28/8/312
2001GU13 Phys.Rev. C63, 044320 (2001) Modified Zimanyi-Moszkowski Model for Finite Nuclei NUCLEAR STRUCTURE 16O, 208Pb; calculated binding energies, radii, single-particle energies. Zimanyi-Moszkowski model with tensor force.
doi: 10.1103/PhysRevC.63.044320
2001GU24 Chinese Physics 10, 805 (2001) Multi-Lambda Matter in a Chiral Hadronic Model
doi: 10.1088/1009-1963/10/9/306
2001GU35 Chin.Phys.Lett. 18, 891 (2001) Tensor Couplings of ω- and ρ-Mesons with Nucleons in a Derivative Scalar Coupling Model for Finite Nuclei NUCLEAR STRUCTURE 16O, 208Pb; calculated single-particle level energies, binding energy, radii and spin-orbit splitting vs tensor coupling.
2001LI59 Nucl.Phys. A695, 353 (2001) Density Dependence of Nucleon Bag Constant, Radius and Mass in an Effective Field Theory Model of QCD
doi: 10.1016/S0375-9474(01)01120-4
2001NO08 Nucl.Phys. A691, 29c (2001) H.Noumi, D.Abe, S.Ajimura, K.Aoki, H.C.Bhang, K.Dobashi, T.Endo, Y.Fujii, T.Fukuda, H.C.Guo, O.Hashimoto, H.Hotchi, E.H.Kim, J.H.Kim, K.Imai, T.Kishimoto, A.Krutenkova, K.Maeda, T.Nagae, M.Nakamura, H.Outa, P.K.Saha, T.Saito, A.Sakaguchi, Y.Sato, R.Sawafta, M.Sekimoto, Y.Shimizu, T.Takahashi, H.Tamura, L.Tang, K.Tanida, T.Watanabe, H.H.Xia, S.H.Zhou, L.H.Zhu, X.F.Zhu First Results on Quasi-Free Σ Production in the (π-, K+) Reactions NUCLEAR REACTIONS H, C, Si, Ni, In, Bi(π-, K+), E at 1.2 GeV/c; measured missing mass spectra; deduced Σ hyperon production features.
doi: 10.1016/S0375-9474(01)00998-8
2000GU02 Phys.Rev. C61, 014307 (2000) Nuclear Surface Properties and Spin-Orbit Potential in a Modified Derivative Coupling Model NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated binding energies, charge radii, spin-orbit splitting; deduced surface effects.
doi: 10.1103/PhysRevC.61.014307
1999GA09 Int.J.Mod.Phys. E8, 39 (1999) The Mean π-Field Should be Calculated in a Relativistic Mean Field Theory for Nuclear Matter
doi: 10.1142/S0218301399000057
1999GU16 J.Phys.(London) G25, 1701 (1999) In-Medium QMC Model Parameters and Quark Condensate in Nuclear Matter
doi: 10.1088/0954-3899/25/1/001
1998GU01 J.Phys.(London) G24, 125 (1998) Quantum Hadrodynamics at Finite Temperature and Density in the Correlation Truncation Approximation
doi: 10.1088/0954-3899/24/1/016
1988XI03 Chin.J.Nucl.Phys. 10, 227 (1988) Xia Yijun, Yang Jingfu, Guo Huachong, Wang Minhua, Xie Bizheng, Wang Shimin Measurement of the Neutron Capture Cross Section of 93Nb NUCLEAR REACTIONS 93Nb(n, γ), E=10-100 keV; measured capture σ(E). Moxon-Rae detectors, 197Au as standard. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32504. Back to query form Note: The following list of authors and aliases matches the search parameter H.Guo: , H.C.GUO, H.R.GUO |