NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = H.Guo

Found 94 matches.

Back to query form



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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32811.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2018GU18      Chin.Phys.C 42, 124101 (2018)

H.-R.Guo, Y.-L.Han, C.-H.Cai

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2017XU05      Phys.Rev. C 96, 024621 (2017)

Y.Xu, H.Guo, Y.Han, Q.Shen

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
Citations: PlumX Metrics


2017XU09      Int.J.Mod.Phys. E26, 1750065 (2017)

Y.Xu, H.Guo, Y.Han, Q.Shen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2014XU01      J.Phys.(London) G41, 015101 (2014)

Y.Xu, H.Guo, Y.Han, Q.Shen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 Greens function method. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064618
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2011HA45      J.Korean Phys.Soc. 59, 859s (2011)

Y.Han, H.Guo, Q.Shen

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
Citations: PlumX Metrics


2011ZH09      Nucl.Sci.Eng. 168, 151 (2011)

Y.Zhang, Y.Han, H.Guo, Q.Shen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32696.


2010GU01      Chin.Phys.Lett. 27, 012401 (2010)

H.-R.Guo, Y.-L.Han, Q.-B.Shen

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
Citations: PlumX Metrics


2010GU03      Phys.Rev. C 81, 044617 (2010)

H.Guo, Y.Han, Q.Shen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010HA19      Nucl.Phys. A834, 495c (2010)

Y.Han, H.Guo, Q.Shen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2009GU05      Nucl.Phys. A823, 83 (2009)

H.Guo, C.-C.Chien, Y.He

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
Citations: PlumX Metrics


2009GU16      Phys.Rev. C 79, 064601 (2009)

H.Guo, Y.Zhang, Y.Han, Q.Shen

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
Citations: PlumX Metrics


2009SH31      Phys.Rev. C 80, 024604 (2009)

Q.-b.Shen, Y.-l.Han, H.-r.Guo

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
Citations: PlumX Metrics


2009ZH02      Nucl.Sci.Eng. 161, 331 (2009)

Y.Zhang, H.Guo, Y.Han, Q.Shen

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
Citations: PlumX Metrics


2008HA15      Nucl.Instrum.Methods Phys.Res. B266, 1943 (2008)

Y.Han, Y.Zhang, H.Guo

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
Citations: PlumX Metrics


2008HA33      Ann.Nucl.Energy 35, 2031 (2008)

Y.Han, Y.Zhang, H.Guo, C.Cai

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
Citations: PlumX Metrics


2008HA38      Nucl.Sci.Eng. 161, 90 (2008)

Y.Han, Y.Zhang, H.Guo

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
Citations: PlumX Metrics


2007CH24      Phys.Rev. C 75, 035806 (2007)

Y.Chen, H.Guo, Y.Liu

Neutrino scattering rates in neutron star matter with Δ isobars

doi: 10.1103/PhysRevC.75.035806
Citations: PlumX Metrics


2007HA52      Nucl.Instrum.Methods Phys.Res. B265, 461 (2007)

Y.Han, Y.Zhang, H.Guo

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2005CH23      Nucl.Phys. A750, 324 (2005)

L.Chang, Y.-X.Liu, H.Guo

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
Citations: PlumX Metrics


2005CH35      Eur.Phys.J. A 24, 211 (2005)

Y.Chen, H.Guo

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
Citations: PlumX Metrics


2005CH72      Phys.Rev. D 72, 094023 (2005)

L.Chang, Y.-x.Liu, H.Guo

Pion-nucleon sigma term in the global color model of QCD

doi: 10.1103/PhysRevD.72.094023
Citations: PlumX Metrics


2005LI07      Chin.Phys.Lett. 22, 298 (2005)

Y.-H.Liang, H.Guo

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2004DO15      Chin.Phys.Lett. 21, 2144 (2004)

B.-G.Dong, H.-C.Guo

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2003DO03      Eur.Phys.J. A 17, 25 (2003)

B.-G.Dong, H.-C.Guo

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
Citations: PlumX Metrics


2003GU04      Phys.Rev. C 67, 024902 (2003)

H.Guo, B.Liu, J.Zhang

Antikaon condensation and in-medium (anti)kaon production in β equilibrium nuclear matter

doi: 10.1103/PhysRevC.67.024902
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2003LI39      Phys.Rev. C 68, 035204 (2003)

Y.-X.Liu, D.-F.Gao, H.Guo

Quark condensates in nuclear matter in the global color symmetry model of QCD

doi: 10.1103/PhysRevC.68.035204
Citations: PlumX Metrics


2002GU23      Chin.Phys.Lett. 19, 1432 (2002)

H.Guo, R.Zhou, Y.-X.Liu

Proton Fraction in Hot Neutron Star Matter with a Chiral Hadronic Model

doi: 10.1088/0256-307X/19/10/311
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2001GU13      Phys.Rev. C63, 044320 (2001)

H.Guo, Y.X.Liu, S.Yang

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
Citations: PlumX Metrics


2001GU24      Chinese Physics 10, 805 (2001)

H.Guo, S.Yang, X.Hu, Y.-X.Liu

Multi-Lambda Matter in a Chiral Hadronic Model

doi: 10.1088/1009-1963/10/9/306
Citations: PlumX Metrics


2001GU35      Chin.Phys.Lett. 18, 891 (2001)

H.Guo, X.Hu

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)

Y.-X.Liu, D.-F.Gao, H.Guo

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2000GU02      Phys.Rev. C61, 014307 (2000)

H.Guo, T.v.Chossy, W.Stocker

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
Citations: PlumX Metrics


1999GA09      Int.J.Mod.Phys. E8, 39 (1999)

C.-Y.Gao, H.Guo, Q.-R.Zhang

The Mean π-Field Should be Calculated in a Relativistic Mean Field Theory for Nuclear Matter

doi: 10.1142/S0218301399000057
Citations: PlumX Metrics


1999GU16      J.Phys.(London) G25, 1701 (1999)

H.Guo

In-Medium QMC Model Parameters and Quark Condensate in Nuclear Matter

doi: 10.1088/0954-3899/25/1/001
Citations: PlumX Metrics


1998GU01      J.Phys.(London) G24, 125 (1998)

H.Guo, C.Li, Q.Wang, Q.Zhang

Quantum Hadrodynamics at Finite Temperature and Density in the Correlation Truncation Approximation

doi: 10.1088/0954-3899/24/1/016
Citations: PlumX Metrics


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