NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = W.Sun Found 75 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
2024YA08 Phys.Rev.Lett. 132, 152502 (2024) X.Yan, Zh.Cheng, A.Abdukerim, Z.Bo, W.Chen, X.Chen, Ch.Cheng, X.Cui, Y.Fan, D.Fang, Ch.Fu, M.Fu, L.Geng, K.Giboni, L.Gu, X.Guo, Ch.Han, K.Han, Ch.He, J.He, D.Huang, Y.Huang, J.Huang, Zh.Huang, R.Hou, Y.Hou, X.Ji, Y.Ju, Ch.Li, J.Li, M.Li, Sh.Li, T.Li, Q.Lin, J.Liu, X.Lu, C.Lu, L.Luo, Y.Luo, W.Ma, Y.Ma, Y.Mao, Y.Meng, X.Ning, B.Pang, N.Qi, Zh.Qian, X.Ren, N.Shaheed, X.Shang, X.Shao, G.Shen, L.Si, W.Sun, A.Tan, Y.Tao, A.Wang, M.Wang, Q.Wang, Sh.Wang, S.Wang, W.Wang, X.Wang, Zh.Wang, Y.Wei, M.Wu, W.Wu, J.Xia, M.Xiao, X.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, Y.Yao, Ch.Yu, Y.Yuan, Zh.Yuan, X.Zeng, D.Zhang, M.Zhang, P.Zhang, Sh.Zhang, Sh.Zhang, T.Zhang, W.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou, Y.Zhou, Y.Zhou, for the PandaX Collaboration Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment RADIOACTIVITY 134Xe(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino and neutrinoless T1/2 limits. Comparison with available data. The cylindrical active volume PandaX-4T dual-phase TPC.
doi: 10.1103/PhysRevLett.132.152502
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
2023WA17 Phys.Lett. B 843, 138034 (2023) W.Wang, C.Lv, X.Zhang, C.Fu, B.Guo, H.Cai, L.Chen, L.Cheng, C.He, J.He, L.Li, X.Xi, D.Yuan, G.Zhang, W.Sun, Z.Zhang, J.Zhang, Y.Ma First measurement of the 7Li(D, n) astrophysical S-factor in laser-induced full plasma NUCLEAR REACTIONS 7Li(d, n), E(cm)<0.7 MeV; measured reaction products, En, In; deduced neutron yields, neutron groups, astrophysical S-factor. The Shenguang-II laser facility, the National Laboratory on High Power Lasers and Physics, Shanghai, China.
doi: 10.1016/j.physletb.2023.138034
2023XI05 Nat.Phys. 19, 904 (2023) T.-Y.Xia, W.-W.Sun, S.Ebser, W.Jiang, G.-M.Yang, H.-M.Yang, H.-M.Zhu, Y.-C.Fu, F.Huang, G.-D.Ming, T.Xia, Z.-T.Lu Atom-trap trace analysis of 41Ca/Ca down to the 1017 level ATOMIC MASSES 41Ca, Ca; measured frequencies; deduced the 41Ca/Ca ratio of a sample and uncertainties, precision. A table-top atom-trap trace analysis (ATTA) system, a magneto-optical trap.
doi: 10.1038/s41567-023-01969-w
2023ZH37 Phys.Rev. C 108, 024310 (2023) X.Y.Zhang, Z.M.Niu, W.Sun, X.W.Xia Nuclear charge radii and shape evolution of Kr and Sr isotopes with the deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Kr, 78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144Sr; calculated binding energy, two-neutron separation energy S(2n), charge radii, quadrupole deformation parameters, potential energy curves. 100Sn; calculated wave function, charge radii as a function of quadrupole deformation parameter. Deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) calculations and DRHBc extended to go beyond mean-field framework by performing a two-dimensional collective Hamiltonian (2DCH). Comparison to experimental data.
doi: 10.1103/PhysRevC.108.024310
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
2022LI28 Few-Body Systems 63, 43 (2022) W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho Progress of Underground Nuclear Astrophysics Experiment JUNA in China NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.
doi: 10.1007/s00601-022-01735-3
2022LV04 Phys.Rev. C 105, 044319 (2022) B.F.Lv, C.M.Petrache, K.K.Zheng, Z.H.Zhang, W.Sun, Z.P.Li, X.T.He, J.Zhang, A.Astier, P.Greenlees, T.Grahn, R.Julin, S.Juutinen, M.Luoma, J.Ojala, J.Pakarinen, J.Partanen, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, H.Tann, J.Uusitalo, G.Zimba, B.Cederwall, O.Aktas, A.Ertoprak, W.Zhang, S.Guo, M.L.Liu, H.J.Ong, Z.Y.Sun, J.G.Wang, X.H.Zhou, I.Kuti, B.M.Nyako, D.Sohler, J.Timar, C.Andreoiu, M.Doncel, D.T.Joss, R.D.Page Refined description of the positive-parity bands and the extent of octupole correlations in 120Ba NUCLEAR REACTIONS 58Ni(64Zn, 2p), E=255 MeV; measured Eγ, Iγ, γγγ-coin, γγ-coin, γ(θ). 120Ba; deduced levels, J, π, DCO ratios, two-point angular correlation (anisotropy) ratios, multipolarity, B(E1), B(E2), B(E3), high-spin states, bands, configurations, alignments, moments of inertia. Comparison with unpaired cranked shell model (CNS), particle number conserving cranked shell-model (PNC-CSM), and Quadrupole and Octupole Collective Hamiltonian based on the Relativistic Hartree-Bogoliubov Model calculations (QOCH-RHB). Systematics of B(E1)/B(E2) of 7- and 9- states in even-even Xe and Ba (A=116-124). JUROGAM3 array and MARA at K130 cyclotron (JYFL).
doi: 10.1103/PhysRevC.105.044319
2022SU16 Chin.Phys.C 46, 064103 (2022) W.Sun, K.-Y.Zhang, C.Pan, X.-H.Fan, S.-Q.Zhang, Z.-P.Li Beyond-mean-field dynamical correlations for nuclear mass table in deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220Nd, 62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122Se, 210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330,332,334,336,338,340,342,344,346,348,350Th; calculated dynamical correlation and rotational correction energies obtained from the cranking approximation, two-neutron seperation energies using the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) with the dynamical correlation energies (DCEs).
doi: 10.1088/1674-1137/ac53fa
2022ZH67 Phys.Rev. C 106, 055803 (2022) L.Y.Zhang, J.Su, J.J.He, R.J.deBoer, D.Kahl, M.Wiescher, D.Odell, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, B.Guo, X.D.Tang, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, J.P.Cheng, W.P.Liu Direct measurement of the astrophysical 19F(p, αγ)16O reaction in a deep-underground laboratory NUCLEAR REACTIONS 19F(p, αγ), E(cm)=72.4-344 keV; measured Eγ, Iγ; deduced astrophysical S-factor, thermonuclear astrophysical reaction rates (range 0.05–1 GK), contributions from different channels. R-matrix analysis with AZURE2 together with a MCMC Bayesian uncertainty estimation. Comparison to other experimental data. 4π BGO γ-array with proton beam from JUNA accelerator at China JinPing underground Laboratory (CJPL).
doi: 10.1103/PhysRevC.106.055803
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
2021PA29 Phys.Rev. C 104, 024331 (2021) C.Pan, K.Y.Zhang, P.S.Chong, C.Heo, M.C.Ho, J.Lee, Z.P.Li, W.Sun, C.K.Tam, S.H.Wong, R.W.-Y.Yeung, T.C.Yiu, S.Q.Zhang Possible bound nuclei beyond the two-neutron drip line in the 50 ≤ Z ≤ 70 region NUCLEAR STRUCTURE 180,182,184,186,188,190,192,194,196,198,200Ba, 220,222,224,226,228,230,232,234,236Sm, 230,232,234,236,238,240,242,244Gd, 242,244,246,248,250,252,254Dy; calculated total energies, neutron Fermi energies, quadrupole deformation parameters β2. 182,184,186,188,190,192,194,196,198Ba, 224,226,228,230,232,234Sm; calculated single-neutron levels around the neutron Fermi energy, pairing energies as function of neutron number. 188Ba; estimated multi-neutron emission and the corresponding half-lives for 4n and 6n emissions as functions of the decay energy. Deformed relativistic Hartree-Bogoliubov in continuum (DRHBc) calculations with density functional PC-PK1. 192,194,196Ba, 192,194,196,198,200,202,204,206,208Ce, 232Sm, 238,240Gd, 250Dy; predicted as bound nuclei beyond the neutron drip line, forming peninsulas of stability in the nuclear landscape.
doi: 10.1103/PhysRevC.104.024331
2021SU11 Appl.Radiat.Isot. 174, 109752 (2021) Production of high-energy neutrons by interaction of a deuteron beam with matter NUCLEAR REACTIONS 12C, 208Pb(p, n), E=256 MeV; 12C(d, n), E=100 MeV; analyzed available data; calculated neutron products σ(θ, E) by the IQMD model.
doi: 10.1016/j.apradiso.2021.109752
2021ZH36 J.Phys.(London) G48, 075101 (2021) X.Zhao, W.Sun, E.Sh.Soukhovitskii, D.S.Martyanov, J.M.Quesada, R.Capote Nucleon scattering analysis with a lane-consistent dispersive optical potential for Hf, W and Ta isotopes NUCLEAR REACTIONS 182,184,186W, 178,180Hf, 181Ta(n, X), (n, n), (n, n'), E<200 MeV; calculated σ, σ(θ); deduced optical model parameters. Comparison with experimental data.
doi: 10.1088/1361-6471/abe280
2021ZH53 Phys.Rev.Lett. 127, 152702 (2021) L.Y.Zhang, J.Su, J.J.He, M.Wiescher, R.J.deBoer, D.Kahl, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, X.D.Tang, H.W.Zhao, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, B.Guo, S.W.Xu, J.Y.Li, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, X.H.Zhou, Y.H.Zhang, F.S.Zhang, Z.G.Hu, H.S.Xu, J.P.Chen, W.P.Liu Direct Measurement of the Astrophysical 19F(p, αγ)16O Reaction in the Deepest Operational Underground Laboratory NUCLEAR REACTIONS 19F(p, α), E(cm)=72.4-188.8 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factors, reaction rates. The China Jinping Underground Laboratory (CJPL), JUNA accelerator.
doi: 10.1103/physrevlett.127.152702
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
2020GU10 Chin.Phys.C 44, 074102 (2020) R.Guo, Y.-H.Liu, J.Li, W.-Ji.Sun, L.Li, Y.-J.Ma Doublet bands at borders of A ≈ 130 island of chiral candidates: Case study of 120I NUCLEAR STRUCTURE 120I; analyzed available data; calculated doublet bands, excitation energies, energy staggering parameter S(I), B(M1)/B(E2), effective angles, and K plots. Comparison with experimental data.
doi: 10.1088/1674-1137/44/7/074102
2020MA41 Eur.Phys.J. A 56, 209 (2020) K.Y.Ma, J.B.Lu, J.Li, Y.J.Ma, D.Yang, W.J.Sun, Q.Y.Yang, X.Guan, J.Q.Wang, H.N.Pan, H.Wang, T.F.Cui, D.M.Zhang, L.H.Zhu, X.G.Wu, Y.Zheng, C.B.Li Candidate magnetic rotational band in 109Ag NUCLEAR REACTIONS 110Pd(7Li, 4nα)109Ag, E=46 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and intensities, J, π, level scheme, bands, momenta, B(M1)/B(E2) ratios.
doi: 10.1140/epja/s10050-020-00213-w
2020MA47 J.Phys.(London) G47, 085106 (2020) K.Y.Ma, J.B.Lu, J.Li, D.Yang, Y.J.Ma, W.J.Sun, J.Q.Wang, Q.Y.Yang, H.Wang, H.N.Pan, D.M.Zhang, L.H.Zhu, X.G.Wu, Y.Zheng, C.B.Li Possible 'stapler' band in 109Ag nucleus NUCLEAR REACTIONS 110Pd(7Li, X)109Ag, E=46 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, multipolarities, J, π, negative-parity band. Comparison with theoretical calculations.
doi: 10.1088/1361-6471/ab920c
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
2020WA07 Eur.Phys.J. A 56, 31 (2020) M.Wang, W.J.Sun, B.H.Sun, J.Li, L.H.Zhu, Y.Zheng, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, C.Xiong, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu The ΔI = 2 bands in 109In: possible antimagnetic rotation NUCLEAR REACTIONS 100Mo(14N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. 109In; deduced levels, J, π, multipolarities, anti-magnetic rotational band, alignments, configurations. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of bands based on πg7/2 orbital in 107,109,111,113In. See also 2018Wa15, a related experiment from the same laboratory.
doi: 10.1140/epja/s10050-020-00039-6
2020ZH21 Phys.Rev. C 101, 064618 (2020) X.Zhao, W.Sun, R.Capote, E.Sh.Soukhovitskih, D.S.Martyanov, J.M.Quesada Dispersive optical model description of nucleon scattering on Pb and Bi isotopes NUCLEAR REACTIONS 208Pb(n, X), E=6-16 MeV; 206,207,208Pb, 209Bi(n, X), E=0.3-200 MeV; calculated total reactions σ(E). 206Pb(n, n), E=2.53, 4.6, 8, 11.01, 13.7, 21.6 MeV; 207Pb(n, n), E=1.47, 2.02, 2.53, 3.04, 3.56, 13.7 MeV; 209Bi(n, n), E=3.99, 5.5, 7.5, 11, 20, 24 MeV; 209Bi(p, p), E=16, 38.7, 55, 57, 65, 153 MeV; calculated elastic scattering differential σ(E, θ). 208Pb(polarized n, n), E=5.969, 6.967, 7.962, 8.958, 9.95, 13.9 MeV; 208Pb(p, p), E=16, 65, 79.8, 98, 160, 182 MeV; 209Bi(n, n), E=3, 3.5, 4, 4.5, 6, 9 MeV; 209Bi(p, p), E=10.76, 12.96, 16, 65, 78, 153 MeV; calculated analyzing power Ay(E, θ). 208Pb(p, n), E=25.8, 35, 45 MeV; 206Pb(p, n), E=25.8 MeV; 209Bi(p, n), E=27 MeV; calculated quasielastic differential σ(E, θ). Modified dispersive optical model potential (DOMP). Comparison with experimental data, and with other theoretical calculations. 208Pb; calculated neutron single-particle energies, spectroscopic factors of valence-neutron-particle states and valence-neutron-hole states. Comparison with experimental data for energies, and with other theoretical calculations.
doi: 10.1103/PhysRevC.101.064618
2019GU25 Phys.Rev. C 100, 034328 (2019) R.Guo, W.-J.Sun, J.Li, D.Yang, Y.Liu, C.Ru, J.Chi Systematic investigations of positive-parity doublet bands with three-quasiparticle configurations in 125, 127, 129, 131Cs NUCLEAR STRUCTURE 125,127,129,131Cs; calculated energies of positive-parity levels, energy staggering parameters, and B(M1)/B(E2) values of doublet bands, single-neutron Routhians, angular momenta as functions of the rotational frequencies, deformation parameters β and γ; assigned configurations to doublet bands. Self-consistent tilted axis cranking relativistic mean-field calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.034328
2019MA48 Phys.Rev. C 100, 014326 (2019) K.Y.Ma, J.B.Lu, J.Li, D.Yang, Y.J.Ma, W.J.Sun, X.Guan, D.M.Zhang, L.H.Zhu, X.G.Wu, Y.Zheng, C.B.Li, Y.Z.Liu Possible antimagnetic rotational band and neutron alignment in 113In NUCLEAR REACTIONS 110Pd(7Li, 4n), E=38, 50 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using HPGe detector array at CIAE-Beijing. 113In; deduced levels, J, π, multipolarities, configurations, alignments, magnetic dipole rotational (shears) bands, antimagnetic rotational bands. Comparison with self-consistent tilted axis cranking relativistic mean-field calculations, with the structure of 111In, and with previous experimental results; predicted B(E2), deformation parameters β2 and γ, and J2/B(E2).
doi: 10.1103/PhysRevC.100.014326
2019SU20 Yuan.Wul.Ping. 36, 144 (2019); Nucl.Phys.Rev. 36, 144 (2019) Beyond-mean-field Study of Octupole Shape Evolution in Neutron-deficient Ba Isotopes NUCLEAR STRUCTURE 114,116,118,120,122,124Ba; calculated binding energies, J, π, potential energy surfaces to study octupole deformation and shape transition using a quadrupole-octupole collective Hamiltonian model.
doi: 10.11804/NuclPhysRev.36.02.144
2019SU22 Phys.Rev. C 100, 044319 (2019) W.Sun, S.Quan, Z.P.Li, J.Zhao, T.Niksic, D.Vretenar Microscopic core-quasiparticle coupling model for spectroscopy of odd-mass nuclei with octupole correlations NUCLEAR STRUCTURE 222,224,226,228Ra; calculated levels, J, π, B(E2), B(E3), relativistic Hartree-Bogoliubov (RHB) deformation energy surfaces in (β2, β3) plane. 223,225,227Ra; calculated levels, J, π, bands, B(E1), B(E2), B(E3), octupole correlations, probabilities of the dominant configurations in wave functions using microscopic core-quasiparticle coupling (CQC) model based on covariant density functional theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.044319
2019ZH56 J.Phys.(London) G46, 055103 (2019) X.Zhao, W.Sun, E.S.Soukhovitskii, D.S.Martyanov, J.M.Quesada, R.Capote Analysis of neutron bound states of 208Pb by a dispersive optical model potential NUCLEAR REACTIONS 208Pb(n, X), (n, n), E<100 MeV; analyzed available data. 208Pb; calculated energy levels, J, π using Bear-Hodgon(BH) and Woods-Saxon potentials, rms radii of valence neutron particle and hole states, σ, σ(θ) using the real dispersive optical model potential for nucleon scattering; deduced optical model parameters.
doi: 10.1088/1361-6471/ab0010
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
2016SU17 Chin.Phys.C 40, 084101 (2016) W.-J.Sun, H.-D.Xu, J.Li, Y.-H.Liu, K.-Y.Ma, D.Yang, J.-B.Lu, Y.-J.Ma Antimagnetic rotation in 108, 110In with tilted axis cranking relativistic mean-field approach NUCLEAR STRUCTURE 108,110In; calculated energy levels, J, π, B(E2), rotational bands. Tilted axis cranking relativistic mean-field theory, comparison with available data.
doi: 10.1088/1674-1137/40/8/084101
2015SU06 J.Phys.(London) B48, 125201 (2015) W.Sun, Q.Wang, Y.Zhang, H.Li, H.Feng, Q.Fan Predicting differential cross sections of electron scattering from polyatomic molecules NUCLEAR REACTIONS N, H, O, C, F, I(E, E), E<50 eV; calculated σ(θ). Comparison with available data.
doi: 10.1088/0953-4075/48/12/125201
2014SU13 Nucl.Data Sheets 118, 191 (2014) W.Sun, R.Li, E.S.Soukhovitskii, J.M.Quesada, R.Capote A Fully Lane-consistent Dispersive Optical Model Potential for Even Fe Isotopes Based on a Soft-rotator Model NUCLEAR REACTIONS 54,56Fe(n, n), E=0-20 MeV; calculated σ using DCCOM (Lane-consistent dispersive CC optical model); deduced optical model parameters. Cross sections compared to data. 54Fe(n, n'), E=9.9-16.9 MeV;54Fe(p, p'), E=10.0=40.0 MeV;56Fe(n, n'), E=9.993 MeV;56Fe(p, p'), E=17.2-65.0 MeV; calculated analyzing power to discrete states. Compared to data. NUCLEAR STRUCTURE 54,58Fe; calculated collective levels, J, π using soft rotator model. Compared with data.
doi: 10.1016/j.nds.2014.04.034
2014YE05 Nucl.Data Sheets 118, 582 (2014) T.Ye, W.Sun, L.Deng, R.She, G.Xiao Prompt Neutron Decay Constants of Reflected Systems
doi: 10.1016/j.nds.2014.04.141
2013LI22 Phys.Rev. C 87, 054611 (2013) R.Li, W.Sun, E.Sh.Soukhovitskih, J.M.Quesada, R.Capote Dispersive coupled-channels optical-model potential with soft-rotator couplings for Cr, Fe, and Ni isotopes NUCLEAR REACTIONS 52Cr, 54,56,58Fe, 59,60,62Ni(n, X), E=0.1-200 MeV; calculated total cross sections and compared with measurements. 54Fe(n, n), E=7.0, 7.96, 8.5, 9.94, 11.0, 11.93, 13.92, 14.7, 16.93, 20.0, 22.0, 24.0, 26.0 MeV; 54Fe(n, n'), E=13.92, 16.93, 20.0, 22.0, 24.0, 26.0 MeV; 56Fe(n, n), E=7.96, 9.94, 11.0, 11.93, 14.0, 14.7, 20.0, 26.0, 55.0, 65.0, 96.0 MeV; 56Fe(n, n'), E=7.96, 9.94, 11.0, 11.93, 13.92, 15.20, 21.1, 26.0 MeV; 54Fe(p, p), E=19.6, 20.4, 24.6, 28.8, 30.4, 35.2, 38.8, 39.7, 40.0, 61.5, 65.0 MeV; 54Fe(p, p'), E=17.9, 18.6, 30.4, 39.7, 40.0, 61.5, 65.0 MeV; 56Fe(p, p), E=7.74, 10.93, 17.2, 19.1, 20.4, 24.6, 30.3, 35.2, 39.8, 61.5, 65.0, 156.0 MeV; 56Fe(p, p'), E=17.2, 19.1, 61.5, 65.0 MeV; 58Fe(p, p), E=6.0, 10.93, 11.66, 22.2, 35.2 MeV; 58Fe(p, p'), E=10.93, 11.66, 17.5, 49.35 MeV; calculated differential σ(θ) and compared with experimental data. 52Cr, 54,56,58Fe, 59,60,62Ni(p, p'), E=1-200 MeV; calculated inelastic cross sections and compared with measurements. 52Cr(p, n), E=17.3, 18.0, 120.0 MeV; 54Fe(p, n), E=23.0, 35.0, 135.0 MeV; 56Fe(p, n), E=17.0, 23.0, 35.2 MeV; 58Fe(p, n), E=23.0, 120.0 MeV; 58Ni(p, n), E=23.0, 32.0, 35.0 MeV; 62Ni(p, n), E=16.0, 22.8, 35.0 MeV; calculated σ(θ) for transition exciting IAS and EAS. 54Fe(polarized p, p), E=10.0, 14.0, 18.6, 30.4, 40.0, 65.0 MeV; 56Fe(polarized p, p), E=5.77, 14.0, 18.6, 24.6, 30.3, 65.0, 179.0 MeV; 58Fe(polarized p, p), E=5.85, 6.51, 14.0, 14.5 MeV; 58Ni(polarized p, p), E=20.9, 30.3, 40.0, 65.0, 172.0 MeV; 54Fe(polarized n, n), (polarized n, n'), E=9.941, 13.9, 13.94, 16.93 MeV; 56Fe(polarized n, n), (polarized n, n'), E=9.993 MeV; 57Fe(polarized p, p), E=5.88, 6.15, 6.51, 14.0 MeV; 58Fe(polarized n, n), E=9.92, 13.91, 16.93 MeV; 54Fe(polarized p, p'), E=10.0, 18.6, 30.4, 40.0 MeV; 56Fe(polarized p, p'), E=17.2, 18.6, 20.4, 24.6, 65.0, 179.0 MeV; 58Ni(polarized p, p'), E=20.4, 24.6, 40.0, 57.5, 60.2, 178.0 MeV; calculated analyzing powers and compared with experimental data, and with TALYS calculations, including DWBA. Derived approximate Lane-consistent dispersive coupled-channels optical potential. NUCLEAR STRUCTURE 54,56,58Fe; analyzed levels, J, π; assigned soft-rotor model (SRM) quantum numbers and Hamiltonian parameters. Coupled-channels optical model analysis using matrix elements derived by the soft-rotator model.
doi: 10.1103/PhysRevC.87.054611
2011SU22 J.Korean Phys.Soc. 59, 947s (2011) A Semi-microscopic Proton Optical Potential for the Mass Range of A = 28 - 90 up to 200 MeV NUCLEAR REACTIONS 32S(p, p), E=15.0, 17.0, 17.5, 19.0, 20.1, 23.0, 25.0, 53 MeV;40Ca(p, p), E=18.07, 30.3, 40.0, 61.4, 65.0, 80.0, 135.0, 152.0, 156.0, 160.0, 201.4 MeV;90Zr(p, p), E=7.97, 12.70, 16.0, 2.50, 40.0, 65.0, 80.0, 100.4, 156.0, 160.0, 185 MeV; calculated σ(θ). 58Ni(p, p), E=16.0, 18.6, 20.4, 24.6, 30.3, 40.0, 65.0, 178.0, 192.0 MeV;90Zr(p, p), E=9.7, 16.0, 40.0, 65.0, 79.6, 134.8, 160.0, 185 MeV; calculated analyzing power. One-body density matrix introduced into single folding model. Comparison to data, JLM and Koning-Delaroche models.
doi: 10.3938/jkps.59.947
2011SU24 J.Korean Phys.Soc. 59, 1088s (2011) Evaluations of Neutron Data for T and 3He with R-Matrix Method NUCLEAR REACTIONS 3H, 3He(n, n), (n, d), (p, p);3H(p, n);3He(p, 2p), (p, 2pn), (n, d), (n, p), (n, np), (n, 2np), (n, γ), E=0-40 MeV; calculated, evaluated σ, σ(θ), covariance matrices using R-matrix; deduced R-matrix parameters.
doi: 10.3938/jkps.59.1088
2011WA36 Chin.Phys.Lett. 28, 112401 (2011) J.Wang, T.Ye, W.-L.Sun, Y.Watanabe, K.Ogata Inclusive Proton Energy Spectra of the Deuteron Induced Reaction NUCLEAR REACTIONS 58Ni(d, xn), (d, xp), E<80 MeV; calculated σ(E), σ(θ, E). Coupled channel method combined with Glauber model, comparison with experimental data.
doi: 10.1088/0256-307X/28/11/112401
2010CH07 Phys.Rev. C 81, 032201 (2010) L.Chang, Y.-X.Liu, C.D.Roberts, Y.-M.Shi, W.-M.Sun, H.-S.Zong Vacuum pseudoscalar susceptibility
doi: 10.1103/PhysRevC.81.032201
2010JI12 Nucl.Phys. A834, 587c (2010) Y.Jiang, N.Li, W.-m.Sun, H.-s.Zong The calculation of quark number susceptibility at finite chemical potential and temperature
doi: 10.1016/j.nuclphysa.2010.01.099
2010WA43 Nucl.Phys. A844, 85c (2010) F.Wang, X.-S.Chen, X.-F.Lu, W.-M.Sun, T.Goldman Gauge invariance and canonical quantization applied in the study of internal structure of gauge field systems
doi: 10.1016/j.nuclphysa.2010.05.019
2009CH14 Phys.Rev. C 79, 035209 (2009) L.Chang, Y.-x.Liu, C.D.Roberts, Y.-m.Shi, W.-m.Sun, H.-s.Zong Chiral susceptibility and the scalar Ward identity
doi: 10.1103/PhysRevC.79.035209
2009LI40 Phys.Rev. C 80, 034909 (2009) X.-y.Li, X.-f.Lu, B.Wang, W.-m.Sun, H.-s.Zong Properties of cold dense nuclear matter based on a nonperturbative approach inspired by chiral perturbation theory
doi: 10.1103/PhysRevC.80.034909
2009OU03 Chin.Phys.Lett. 26, 052501 (2009) L.Ou, Z.-X.Li, X.-Z.Wu, W.-L.Sun Disentangling the Effects of Thickness of the Neutron Skin and Symmetry Potential in Nucleon Induced Reactions on Sn Isotopes NUCLEAR REACTIONS 112Sn, 132Sn, 112Cd, 132Ba(n, X), E=100 MeV; 112Sn, 132Sn, 112Cd, 132Ba(p, X), E=100 MeV; calculated σ for target nuclei with normal and enlarged neutron skin. Improved molecular dynamics model.
doi: 10.1088/0256-307X/26/5/052501
2008HA28 J.Phys.(London) G35, 095103 (2008) L.Hao, W.Sun, E.Sh.Soukhovitskii A global dispersive coupled-channel potential for the A = 24-122 mass range up to 200 MeV NUCLEAR REACTIONS 24Mg, 28Si, 32S, 40Ca, 48Ti, 52Cr, 56Fe, 58Ni, 90Zr, 98Mo, 120Sn(n, X), E=1 keV-200 MeV; 28Si, 40Ca, 56Fe, 90Zr, 120Sn(p, X), E=1 keV-200 MeV; analyzed σ, σ(θ), analyzing power Ay(θ); deduced global optical model parameters; dispersive coupled channel optical model approach.
doi: 10.1088/0954-3899/35/9/095103
2008JI07 Phys.Rev. C 78, 025214 (2008) Yu.Jiang, Y.-m.Shi, H.-t.Feng, W.-m.Sun, H.-s.Zong Quark-meson vertices and pion properties at finite chemical potential
doi: 10.1103/PhysRevC.78.025214
2006SU18 Chin.Phys.Lett. 23, 3234 (2006) Chemical Potential Dependence of Two-Quark Condensates
doi: 10.1088/0256-307X/23/12/031
2006ZO01 Phys.Rev. C 73, 035206 (2006) Modified approach for calculating axial vector vacuum susceptibility
doi: 10.1103/PhysRevC.73.035206
2005HO26 Phys.Rev. C 72, 034901 (2005) F.-y.Hou, L.Chang, W.-m.Sun, H.-s.Zong, Y.-x.Liu New method for numerically solving the chemical potential dependence of the dressed quark propagator
doi: 10.1103/PhysRevC.72.034901
2005ZO01 Phys.Rev. C 71, 015205 (2005) H.-s.Zong, L.Chang, F.-y.Hou, W.-m.Sun, Y.-x.Liu New approach for calculating the dressed quark propagator at finite chemical potential
doi: 10.1103/PhysRevC.71.015205
2005ZO03 Phys.Rev. C 72, 035202 (2005) H.-s.Zong, F.-y.Hou, W.-m.Sun, J.-l.Ping, E.-g.Zhao Modified approach for calculating vacuum susceptibility
doi: 10.1103/PhysRevC.72.035202
2004CH19 Phys.Rev. C 69, 045201 (2004) X.-S.Chen, D.Qing, W.-M.Sun, H.-S.Zong, F.Wang Spin-orbital structure of the nucleon magnetic moment
doi: 10.1103/PhysRevC.69.045201
2004CH37 Phys.Rev. C 70, 015201 (2004) X.-S.Chen, R.G.E.Timmermans, W.-Mi.Sun, H.-S.Zong, F.Wang Examination of the strangeness contribution to the nucleon magnetic moment NUCLEAR STRUCTURE 1n, 1H; calculated strangeness contribution to magnetic moment. Meson cloud model.
doi: 10.1103/PhysRevC.70.015201
2003SU31 J.Nucl.Sci.Technol.(Tokyo) 40, 635 (2003) W.Sun, Y.Watanabe, E.Sh.Sukhovitskii, O.Iwamoto, S.Chiba Coupled-Channels Analysis of Nucleon Interaction Data of 28, 30Si up to 200 MeV Based on the Soft Rotator Model NUCLEAR REACTIONS 28Si(n, n), (n, n'), (p, p), (p, p'), E=14-180 MeV; 30Si(p, p'), E=52 MeV; calculated σ(θ). 28Si(p, X), E=5-200 MeV; calculated reaction σ. Soft rotator model, coupled-channels approach, comparison with data. NUCLEAR STRUCTURE 28,30Si; calculated levels, J, π. Soft rotator model.
doi: 10.1080/18811248.2003.9715401
1999OG12 Phys.Rev. C60, 054605 (1999); Erratum Phys.Rev. C63, 019902 (2001) K.Ogata, M.Kawai, Y.Watanabe, W.Sun, M.Kohno Theoretical Modification on Semiclassical Distorted Wave Model and Its Application to the Study of Spin Observables NUCLEAR REACTIONS 90Zr(p, p'X), (p, nX), E=160 MeV; 58Ni(p, p'X), E=80 MeV; calculated σ(E, θ), spin observables. Extended semiclassical distorted wave model, comparisons with data.
doi: 10.1103/PhysRevC.60.054605
1999SU15 Phys.Rev. C60, 064605 (1999); Erratum Phys.Rev. C63, 019903 (2001) W.Sun, Y.Watanabe, M.Kohno, K.Ogata, M.Kawai Semiclassical Distorted Wave Model with Wigner Transform of One-Body Density Matrix NUCLEAR REACTIONS 90Zr(p, p'X), E=80, 160 MeV; calculated σ(E, θ); deduced target nucleon momentum effects. Semiclassical distorted wave model, finite range single particle potential. Comparison with data, other models.
doi: 10.1103/PhysRevC.60.064605
1999WA07 Phys.Rev. C59, 2136 (1999); Erratum Phys.Rev. C63, 019901 (2001) Y.Watanabe, R.Kuwata, W.Sun, M.Higashi, H.Shinohara, M.Kohno, K.Ogata, M.Kawai Semiclassical Distorted Wave Model Analysis of Multistep Direct (p, p'x) and (p, nx) Reactions to the Continuum NUCLEAR REACTIONS 90Zr(p, p'X), (p, nX), E=80, 120, 160 MeV; 58Ni(p, p'X), E=65, 120 MeV; 209Bi(p, p'X), E=62 MeV; calculated σ(E, θ); deduced role of three-step processes. Extended semiclassical distorted wave model. Comparison with data, other models.
doi: 10.1103/PhysRevC.59.2136
1997SH05 Phys.Rev. C55, 614 (1997) Scalar-Isoscalar Meson Exchange in the Calculation of the Nucleon-Nucleon Interaction
doi: 10.1103/PhysRevC.55.614
1996CE05 Phys.Rev. C54, 487 (1996) L.S.Celenza, C.M.Shakin, W.-D.Sun Calculation of the Nucleon-Nucleon Interaction Due to Vector-Meson Exchange
doi: 10.1103/PhysRevC.54.487
1996GA04 Phys.Rev. C53, 1374 (1996) S.-F.Gao, C.M.Shakin, W.-D.Sun Many-Body Theory of ρ-ω Mixing
doi: 10.1103/PhysRevC.53.1374
1996GA07 Phys.Rev. C53, 1936 (1996) S.-F.Gao, L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda Bosonization in the Presence of Confinement: Calculation of the nucleon-nucleon interaction
doi: 10.1103/PhysRevC.53.1936
1996SH07 Phys.Rev. C53, 3152 (1996) Use of Quark Wave Functions in the Calculation of Structure Functions of Mesons
doi: 10.1103/PhysRevC.53.3152
1996SH14 Phys.Rev. C54, 1414 (1996) Gauge Invariance and Confinement in a Generalized Nambu-Jona-Lasinio Model
doi: 10.1103/PhysRevC.54.1414
1996SZ08 Few-Body Systems 20, 93 (1996) J.Szweda, L.S.Celenza, C.M.Shakin, W.-D.Sun Quark-Quark Correlations in the Nucleon in a Generalized Nambu-Jona-Lasinio Model NUCLEAR STRUCTURE 1H, 1n; calculated μ. Generalized Nambu-Jona-Lasinio model, quark-quark correlations.
doi: 10.1007/s006010050034
1995CE02 Phys.Rev. C51, 937 (1995) L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda Use of the Nambu-Jona-Lasino Model in the Calculation of the Density Dependence of Four-Quark Condensates
doi: 10.1103/PhysRevC.51.937
1995CE05 Phys.Rev. C51, 3372 (1995) L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda Nuclear Many-Body Theory for the Study of QCD Sum Rules in Matter
doi: 10.1103/PhysRevC.51.3372
1995SH05 Phys.Rev. C51, 2171 (1995) Deep-Inelastic Scattering from the Pion and the Choice of Phenomenological Wave Functions
doi: 10.1103/PhysRevC.51.2171
1995SH32 Phys.Rev. C52, 3353 (1995) C.M.Shakin, W.-D.Sun, J.Szweda Generalized Nambu-Jona-Lasinio Model in a Study of the Boson-Exchange Model of Nuclear Forces
doi: 10.1103/PhysRevC.52.3353
1995SH33 Phys.Rev. C52, 3502 (1995) C.M.Shakin, W.-D.Sun, J.Szweda Meson-Mode Mixing in the Calculation of the Nucleon-Nucleon Interaction
doi: 10.1103/PhysRevC.52.3502
1994SH03 Phys.Rev. C49, 1185 (1994) Properties of the rho Meson in Nuclear Matter
doi: 10.1103/PhysRevC.49.1185
1994SH22 Phys.Rev. C50, 2553 (1994) Structure Function of Off-Mass-Shell Pions and the Calculation of the Sullivan Process
doi: 10.1103/PhysRevC.50.2553
1993CE10 Int.J.Mod.Phys. E2, 603 (1993) L.S.Celenza, C.M.Shakin, W.-D.Sun, J.Szweda, X.Zhu Scalar-Isoscalar Correlator in a Phenomenological Coupled-Channel Quark Model
doi: 10.1142/S0218301393000261
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