NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = X.Sun Found 172 matches. Showing 1 to 100. [Next]2024IM02 Phys.Lett. B 850, 138470 (2024) N.Imai, M.Dozono, S.Michimasa, T.Sumikama, S.Ota, S.Hayakawa, J.W.Hwang, K.Iribe, C.Iwamoto, S.Kawase, K.Kawata, N.Kitamura, S.Masuoka, K.Nakano, P.Schrock, D.Suzuki, R.Tsunoda, K.Wimmer, D.S.Ahn, O.Beliuskina, N.Chiga, N.Fukuda, E.Ideguchi, K.Kusaka, H.Miki, H.Miyatake, D.Nagae, S.Ohmika, M.Ohtake, H.J.Ong, H.Otsu, H.Sakurai, H.Shimizu, Y.Shimizu, X.Sun, H.Suzuki, M.Takaki, H.Takeda, S.Takeuchi, T.Teranishi, Y.Watanabe, Y.X.Watanabe, K.Yako, H.Yamada, H.Yamaguchi, L.Yang, R.Yanagihara, Y.Yanagisawa, K.Yoshida, S.Shimoura Neutron capture reaction cross-section of 79Se through the 79Se(d, p) reaction in inverse kinematics NUCLEAR REACTIONS 2H(77Se, p), (79Se, p), E=20 MeV/nucleon; measured reaction products, Eγ, Iγ. 78,80Se; deduced γ-ray energies, γ-emission probabilities, σ, isomer ratio. Comparison with available data, TALYS and code DWUCK5 calculations. The surrogate-ratio method, the RI Beam Factory operated by the RIKEN Nishina Center and the Center for Nuclear Studies (CNS), University of Tokyo, by employing the novel "optimized energy degrading optics" (OEDO) for radioactive isotope (RI) beams.
doi: 10.1016/j.physletb.2024.138470
2024ST02 Nuovo Cim. C 47, 39 (2024) L.Stuhl, M.Sasano, J.Gao, Y.Hirai, K.Yako, T.Wakasa, D.S.Ahn, H.Baba, A.I.Chilug, S.Franchoo, Y.Fujino, N.Fukuda, J.Gibelin, I.S.Hahn, Z.Halasz, T.Harada, M.N.Harakeh, D.Inomoto, T.Isobe, H.Kasahara, D.Kim, G.G.Kiss, T.Kobayashi, Y.Kondo, Z.Korkulu, S.Koyama, Y.Kubota, A.Kurihara, H.N.Liu, M.Matsumoto, S.Michimasa, H.Miki, M.Miwa, T.Motobayashi, T.Nakamura, M.Nishimura, H.Otsu, V.Panin, S.Park, A.T.Saito, H.Sakai, H.Sato, T.Shimada, Y.Shimizu, S.Shimoura, A.Spiridon, I.C.Stefanescu, X.Sun, Y.L.Sun, H.Suzuki, E.Takada, Y.Togano, T.Tomai, L.Trache, D.Tudor, T.Uesaka, H.Yamada, Z.Yang, M.Yasuda, K.Yoneda, K.Yoshida, J.Zenihiro, N.Zhang Study of Gamow-Teller giant resonance in 11Li drip-line nucleus NUCLEAR REACTIONS 1H(11Li, n), E=182 MeV/nucleon; measured reaction products, En, In. 11Li, 11Be; deduced level energies, decay channels, Gamow-Teller (GT) transitions. The neutron detector array PANDORA and the SAMURAI spectrometer, RI Beam Factory (RIBF) of RIKEN Nishina Center.
doi: 10.1393/ncc/i2024-24039-6
2024XU04 Chin.Phys.C 48, 024106 (2024) Y.-L.Xu, X.-W.Su, Zh.-H.Sun, Y.-L.Han, X.-J.Sun, D.-H.Zhang, Ch.-H.Cai Description of elastic scattering for 7Li-induced reactions on 1p-shell nuclei NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 15N, 16O(7Li, 7Li), E=4.5-131.8 MeV; analyzed available data; deduced σ(θ), the global phenomenological optical potentials (GPOPs), the contribution of elastic transfer by the distorted wave Born approximation (DWBA) method.
doi: 10.1088/1674-1137/ad1924
2024ZH13 Chin.Phys.C 48, 014107 (2024) R.-Y.Zheng, X.-X.Sun, G.-f.Shen, L.-Sh.Geng Evolution of N = 20, 28, 50 shell closures in the 20≤Z≤30 region in deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE Z=20-30; calculated charge radii, two-neutron separation energies, two-neutron gaps, quadrupole deformations, and single-particle levels with the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) with the density functional PC-PK1. Comparison with available data.
doi: 10.1088/1674-1137/ad0bf2
2023CH23 Phys.Rev. C 107, 054306 (2023) J.Chen, M.Liu, C.Yuan, S.Chen, N.Shimizu, X.Sun, R.Xu, Y.Tian Shell-model-based investigation on level density of Xe and Ba isotopes NUCLEAR STRUCTURE 131,132,133,134Sn, 132,133,134,135Sb, 133,134,135,136Te, 134,135,136,137I, 135,136,137,138Xe, 136,137,138,139Cs, 137,138,139,140Ba; calculated one-neutron separation energy S(n). 132,133,134Sn, 132,133,134,135Sb, 134,135,136Te, 135,136,137I, 136,137,138Xe, 137,138,139Cs, 138,139,140Ba; calculated two-neutron separation energies S(2n). 134, ,136,138Xe, 134,136,138,140Ba, 128,129,130,134,135,136Sn, 131,135Sb, 132,134,136Te, 133,135,137I, 135,137,139Cs, 139La; calculated levels, J, π. 133,134,135,136,137Xe, 134,135,136,137,138,139Ba; calculated nuclear level densities (NLD), cumulative number of levels spin distributions. 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La; calculated effective single particle energy for proton and neutron orbits with and without the consideration of tensor part in two-body matrix elements. 133,134,135,136,137Xe; calculated spin distribution , parity ratios, spin cut-off parameter. Configuration-interaction shell model with a unified effective nuclear force. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.054306
2023SU02 Phys.Rev. C 107, L011601 (2023) Microscopic study of fusion reactions with a weakly bound nucleus: Effects of deformed halo NUCLEAR REACTIONS 232Th(14C, X), (15C, X), E(cm)=50-70 MeV; calculated fusion σ(E), intranuclear potential. 232Th(15C, 14C), E=54 MeV; calculated one-neutron transfer probability for 49 different orientations. Time-dependent density functional theory (TDDFT). Comparison to experimental data. NUCLEAR STRUCTURE 14,15C; calculated two-dimensional density distribution of the ground state.
doi: 10.1103/PhysRevC.107.L011601
2023SU05 Phys.Rev. C 107, 064609 (2023) Microscopic study of the hot-fusion reaction 48Ca + 238U with the constraints from time-dependent Hartree-Fock theory NUCLEAR REACTIONS 238U(48Ca, X), E(cm)=180-215 MeV; calculated capture σ(E), fusion σ(E), orientation-averaged fusion σ(E), fusion probabilities, injection distances, separation distance of centers of mass of two fragments with zero conjugate momenta, internuclear potentials between 48Ca and 238U for different orientations, density distributions. 238U(48Ca, 3n), (48Ca, 4n), E(cm)=18-205 MeV; calculated evaporation-residue σ(E). Calculations utilizing microscopic descriptions of the ground state with static Hartree-Fock calculations and reaction dynamic using time-dependent Hartree-Fock (TDHF) theory, in combination with coupled-channel and fusion-by-diffusion models. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.064609
2023XI09 Phys.Lett. B 845, 138160 (2023) Y.Xiao, S.-Z.Xu, R.-Y.Zheng, X.-X.Sun, L.-S.Geng, S.-S.Zhang One-proton emission from 148-151Lu in the DRHBc+WKB approach RADIOACTIVITY 148,149,150,151Lu(p); analyzed available data; deduced proton-nucleus potential from the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc), oblate deformation, T1/2, the DRHBc + WKB approach provides a new alternative method to evaluate the half-lives of well-deformed proton emitters.
doi: 10.1016/j.physletb.2023.138160
2023ZH15 Phys.Rev. C 107, L041303 (2023) K.Y.Zhang, P.Papakonstantinou, M.-H.Mun, Y.Kim, H.Yan, X.-X.Sun Collapse of the N=28 shell closure in the newly discovered 39Na nucleus and the development of deformed halos towards the neutron dripline NUCLEAR STRUCTURE 39Na; calculated S(n), single-neutron levels, J, π, quadrupole deformation, rms radius. 31,33,35,37,39,41Na; calculated neutron density distributions. Pointed that 39Na could be single nucleus with the coexistence of several exotic structures, including the quenched N=28 shell closure, Borromean structure, deformed halo, and between the core and the halo. Discussed the microscopic mechanisms behind the shape decoupling phenomenon and the development of halos towards dripline. Deformed relativistic Hartree-Bogoliubov theory in continuum.
doi: 10.1103/PhysRevC.107.L041303
2023ZO01 Chin.Phys.C 47, 044101 (2023) F.Zou, X.Sun, K.Zhang, H.Chen, J.Yan, J.Tian, Y.Cui Pre-neutron fragment mass yields for 235U(n, f) and 239Pu(n, f) reactions at incident energies from thermal up to 20 MeV NUCLEAR REACTIONS 235U, 239Pu(n, F), E<20 MeV; calculated pre-neutron fragment mass yields at incident energies from thermal up to 20 MeV using an empirical fission potential (EFP) model, the potential parameters of which are obtained from the measured data.
doi: 10.1088/1674-1137/acb910
2022CU09 Phys.Rev. C 106, 065506 (2022) C.Cude-Woods, F.M.Gonzalez, E.M.Fries, T.Bailey, M.Blatnik, N.B.Callahan, J.H.Choi, S.M.Clayton, S.A.Currie, M.Dawid, B.W.Filippone, W.Fox, P.Geltenbort, E.George, L.Hayen, K.P.Hickerson, M.A.Hoffbauer, K.Hoffman, A.T.Holley, T.M.Ito, A.Komives, C.-Y.Liu, M.Makela, C.L.Morris, R.Musedinovic, C.O'Shaughnessy, R.W.Pattie, J.Ramsey, D.J.Salvat, A.Saunders, E.I.Sharapov, S.Slutsky, V.Su, X.Sun, C.Swank, Z.Tang, W.Uhrich, J.Vanderwerp, P.Walstrom, Z.Wang, W.Wei, A.R.Young Fill and dump measurement of the neutron lifetime using an asymmetric magneto-gravitational trap RADIOACTIVITY 1NN(β-); measured number of trapped neutrons; deduced free neutron lifetime T1/2. Comparison to previous most precise experimental data. Asymmetric magneto-gravitational trap at Los Alamos Ultracold Neutron Facility.
doi: 10.1103/PhysRevC.106.065506
2022DE15 Chin.Phys.C 46, 061001 (2022) J.-G.Deng, H.-F.Zhang, X.-D.Sun New behaviors of α-particle preformation factors near doubly magic 100Sn RADIOACTIVITY 104,106,108,110Te, 108,110,112Xe, 114Ba, 212,214,216,218Po, 212,214,216,218,220,222Rn, 214,216,218,220,222,224,226Ra(α); calculated T1/2 within the generalized liquid drop model. Comparison with available data.
doi: 10.1088/1674-1137/ac5a9f
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
2022HA10 Phys.Rev. C 105, 044302 (2022) J.X.Han, Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, Z.H.Yang, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song Observation of the π2σ2-bond linear-chain molecular structure in 16C NUCLEAR REACTIONS 2H(16C, X)16C/2H/1H/2H/3H/3He/4He/5He/6He/6Li/7Li/8Li/9Li/7Be/8Be/9Be/10Be/11Be/12Be, E=23.5 MeV/nucleon; measured reaction products, recoil 2H, 8Be and other outgoing particles; deduced Q-value spectra for breakup of excited states of 16C into 4He+12Be and 6He+10Be channels, angular correlation between 4He and 12Be decay fragments from the 16.5 MeV resonance in 16C, and 6He and 10Be fragments from the 19.4 MeV resonance in 16C. 16C; deduced excitation energy spectra reconstructed from 4He+12Be+2 H and 6He+10Be+2H channels, levels, resonances, total width. Comparison with previous experimental data, and with antisymmetrized molecular dynamics (AMD) theoretical calculations. Secondary 16C beam produced in 9Be(18O, X), E=59.6 MeV/nucleon primary reaction at the HIRFL-RIBLL facility in Lanzhou.
doi: 10.1103/PhysRevC.105.044302
2022HU16 Int.J.Mod.Phys. E31, 2250072 (2022) J.Hu, S.Wang, X.Sun, Y.Han, J.Zhang Effects of energy levels of the compound nucleus on particle emission for the 6Li(n, t), 3He(n p), and 7Be(n, p) reactions NUCLEAR REACTIONS 6Li(n, t), 3He(n, p), 7Be(n, p), E<10 MeV; calculated σ using the improved knockout model. Comparison with ENDF/B-VIII.0, JENDL-4.0, EAF-2010 libraries and experimental data.
doi: 10.1142/S0218301322500720
2022SU04 Int.J.Mod.Phys. E31, 2250001 (2022) Z.-H.Sun, Y.-L.Xu, X.-J.Sun, Y.-L.Han, C.-H.Cai Global phenomenological optical model potential for 14N-nucleus elastic scattering NUCLEAR REACTIONS 24Mg, 27Al, 28,29Si, 32S, 40Ca, 56Fe, 59Co, 58,62Ni, 70,74Ge, 90Zr, 92,100Mo, 118Sn, 208Pb(14N, 14N), E<100 MeV; analyzed available data; deduced global optical model potential parameters, σ, σ(θ).
doi: 10.1142/S021830132250001X
2022SU07 Phys.Rev. C 105, 034601 (2022) Microscopic study of the fusion reactions 40, 48Ca+78Ni and the effect of the tensor force NUCLEAR REACTIONS 78Ni(40Ca, X), (48Ca, X), E(cm)=70, 80, 90 MeV; calculated internuclear potentials, fusion σ. Dynamic density-constrained time-dependent Hartree-Fock (DC-TDHF) and static Hartree-Fock theory. Discussed role of tensor force in the fusion of nuclei.
doi: 10.1103/PhysRevC.105.034601
2022SU09 Phys.Rev. C 105, 044312 (2022) Finite amplitude method on the deformed relativistic Hartree-Bogoliubov theory in continuum: The isoscalar giant monopole resonance in exotic nuclei NUCLEAR STRUCTURE 40,42,44,46,48,68,80Ca, 208Pb; calculated isoscalar giant monopole resonance, monopole strength distributions. 40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80Ca; calculated energy weighted sum rule for isoscalar giant monopole resonance. 200Nd; calculated proton and neutron transition densities of the soft monopole mode in prolate and oblate cases, potential energy curve, features of the isoscalar giant monopole resonance built on ground state and prolate isomer state, monopole strength distribution. Finite amplitude method based on the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc-FAM). Comparison to available experimental data.
doi: 10.1103/PhysRevC.105.044312
2022SU10 Phys.Rev. C 105, 054610 (2022) Microscopic study of compound-nucleus formation in cold-fusion reactions NUCLEAR REACTIONS 208Pb(48Ca, X), E=160-220 MeV; 208Pb(50Ti, X), E=180-230 MeV; 208Pb(54Cr, X), E=190-235 MeV; calculated capture and fusion σ(E), effective fusion probabilities, injection parameters. The time-dependent Hartree-Fock (TDHF) approach. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.054610
2022SU20 Phys.Rev. C 106, 024334 (2022) Triaxiality-induced monopole-quadrupole-hexadecupole coupling in the isoscalar giant resonances of 86Ge NUCLEAR STRUCTURE 64,74,86Ge; calculated potential energy surfaces (β, γ) plane, monopole strength distributions. 86Ge; calculated isoscalar giant monopole resonance structure, isoscalar giant quadrupole resonance structure, isoscalar giant hexadecupole resonance structure, transition densities, single neutron levels. Pointed on evidence for the monopole-quadrupole-hexadecupole coupling. Quasiparticle finite amplitude method (QFAM) based on the covariant density functional (CDFT) theory DD-ME2 and a separable pairing force.
doi: 10.1103/PhysRevC.106.024334
2022WA08 Chin.Phys.C 46, 024107 (2022) X.-Q.Wang, X.-X.Sun, S.-G.Zhou Microscopic study of higher-order deformation effects on the ground states of superheavy nuclei around 270Hs NUCLEAR STRUCTURE 264,266,268,270,272,274,276Hs, 266Rf, 268Sg, 272Ds; calculated binding energies, energy levels, J, π, deformation parameters using the deformation relativistic Hartree-Bogoliubov (DRHBc) theory.
doi: 10.1088/1674-1137/ac3904
2022XU14 Int.J.Mod.Phys. E31, 2250093 (2022) Y.Xu, X.Su, Y.Han, X.Sun, D.Zhang, C.Cai Optical potential for the elastic scattering of 6Li projectile on 1p-shell nuclei NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 12,13,14C, 15N, 16,18O(6Li, 6Li), E=2-210 MeV; analyzed available data; deduced σ(θ), a set of global optical potential parameters by fitting the experimental data of elastic scattering angular distributions.
doi: 10.1142/S0218301322500938
2022ZH74 Sci.China: Phys.Mech.Astron. 65, 262011 (2022) S.-Y.Zhong, S.-S.Zhang, X.-X.Sun, M.S.Smith Study of the deformed halo nucleus 31Ne with Glauber model based on microscopic self-consistent structures NUCLEAR STRUCTURE 26,27,28,29,30,31Ne; calculated two-dimensional neutron density functions, averaged-angle neutron densities, single neutron levels, inclusive parallel momentum distributions. The deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc). NUCLEAR REACTIONS 12C(26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), E=240 MeV/nucleon; calculated σ using DRHBc and RAB model. Comparison with experimental data.
doi: 10.1007/s11433-022-1894-6
2021AB12 Phys.Rev. C 104, L061901 (2021) M.S.Abdallah, B.E.Aboona, J.Adam, L.Adamczyk, J.R.Adams, J.K.Adkins, G.Agakishiev, I.Aggarwal, M.M.Aggarwal, Z.Ahammed, I.Alekseev, D.M.Anderson, A.Aparin, E.C.Aschenauer, M.U.Ashraf, F.G.Atetalla, A.Attri, G.S.Averichev, V.Bairathi, W.Baker, J.G.Ball Cap, K.Barish, A.Behera, R.Bellwied, P.Bhagat, A.Bhasin, J.Bielcik, J.Bielcikova, I.G.Bordyuzhin, J.D.Brandenburg, A.V.Brandin, I.Bunzarov, J.Butterworth, X.Z.Cai, H.Caines, M.Calderon de la Barca Sanchez, D.Cebra, I.Chakaberia, P.Chaloupka, B.K.Chan, F.-H.Chang, Z.Chang, N.Chankova-Bunzarova, A.Chatterjee, S.Chattopadhyay, D.Chen, J.Chen, J.H.Chen, X.Chen, Z.Chen, J.Cheng, M.Chevalier, S.Choudhury, W.Christie, X.Chu, H.J.Crawford, M.Csanad, M.Daugherity, T.G.Dedovich, I.M.Deppner, A.A.Derevschikov, A.Dhamija, L.Di Carlo, L.Didenko, P.Dixit, X.Dong, J.L.Drachenberg, E.Duckworth, J.C.Dunlop, N.Elsey, J.Engelage, G.Eppley, S.Esumi, O.Evdokimov, A.Ewigleben, O.Eyser, R.Fatemi, F.M.Fawzi, S.Fazio, P.Federic, J.Fedorisin, C.J.Feng, Y.Feng, P.Filip, E.Finch, Y.Fisyak, A.Francisco, C.Fu, L.Fulek, C.A.Gagliardi, T.Galatyuk, F.Geurts, N.Ghimire, A.Gibson, K.Gopal, X.Gou, D.Grosnick, A.Gupta, W.Guryn, A.I.Hamad, A.Hamed, Y.Han, S.Harabasz, M.D.Harasty, J.W.Harris, H.Harrison, S.He, W.He, X.H.He, Y.He, S.Heppelmann, S.Heppelmann, N.Herrmann, E.Hoffman, L.Holub, Y.Hu, H.Huang, H.Z.Huang, S.L.Huang, T.Huang, X.Huang, Y.Huang, T.J.Humanic, G.Igo, D.Isenhower, W.W.Jacobs, C.Jena, A.Jentsch, Y.Ji, J.Jia, K.Jiang, X.Ju, E.G.Judd, S.Kabana, M.L.Kabir, S.Kagamaster, D.Kalinkin, K.Kang, D.Kapukchyan, K.Kauder, H.W.Ke, D.Keane, A.Kechechyan, M.Kelsey, Y.V.Khyzhniak, D.P.Kikola, C.Kim, B.Kimelman, D.Kincses, I.Kisel, A.Kiselev, A.G.Knospe, H.S.Ko, L.Kochenda, L.K.Kosarzewski, L.Kramarik, P.Kravtsov, L.Kumar, S.Kumar, R.Kunnawalkam Elayavalli, J.H.Kwasizur, R.Lacey, S.Lan, J.M.Landgraf, J.Lauret, A.Lebedev, R.Lednicky, J.H.Lee, Y.H.Leung, C.Li, C.Li, W.Li, X.Li, Y.Li, X.Liang, Y.Liang, R.Licenik, T.Lin, Y.Lin, M.A.Lisa, F.Liu, H.Liu, H.Liu, P.Liu, T.Liu, X.Liu, Y.Liu, Z.Liu, T.Ljubicic, W.J.Llope, R.S.Longacre, E.Loyd, N.S.Lukow, X.F.Luo, L.Ma, R.Ma, Y.G.Ma, N.Magdy, D.Mallick, S.Margetis, C.Markert, H.S.Matis, J.A.Mazer, N.G.Minaev, S.Mioduszewski, B.Mohanty, M.M.Mondal, I.Mooney, D.A.Morozov, A.Mukherjee, M.Nagy, J.D.Nam, Md.Nasim, K.Nayak, D.Neff, J.M.Nelson, D.B.Nemes, M.Nie, G.Nigmatkulov, T.Niida, R.Nishitani, L.V.Nogach, T.Nonaka, A.S.Nunes, G.Odyniec, A.Ogawa, S.Oh, V.A.Okorokov, B.S.Page, R.Pak, J.Pan, A.Pandav, A.K.Pandey, Y.Panebratsev, P.Parfenov, B.Pawlik, D.Pawlowska, H.Pei, C.Perkins, L.Pinsky, R.L.Pinter, J.Pluta, B.R.Pokhrel, G.Ponimatkin, J.Porter, M.Posik, V.Prozorova, N.K.Pruthi, M.Przybycien, J.Putschke, H.Qiu, A.Quintero, C.Racz, S.K.Radhakrishnan, N.Raha, R.L.Ray, R.Reed, H.G.Ritter, M.Robotkova, O.V.Rogachevskiy, J.L.Romero, D.Roy, L.Ruan, J.Rusnak, N.R.Sahoo, H.Sako, S.Salur, J.Sandweiss, S.Sato, W.B.Schmidke, N.Schmitz, B.R.Schweid, F.Seck, J.Seger, M.Sergeeva, R.Seto, P.Seyboth, N.Shah, E.Shahaliev, P.V.Shanmuganathan, M.Shao, T.Shao, A.I.Sheikh, D.Shen, S.S.Shi, Y.Shi, Q.Y.Shou, E.P.Sichtermann, R.Sikora, M.Simko, J.Singh, S.Singha, M.J.Skoby, N.Smirnov, Y.Sohngen, W.Solyst, P.Sorensen, H.M.Spinka, B.Srivastava, T.D.S.Stanislaus, M.Stefaniak, D.J.Stewart, M.Strikhanov, B.Stringfellow, A.A.P.Suaide, M.Sumbera, B.Summa, X.M.Sun, X.Sun, Y.Sun, Y.Sun, B.Surrow, D.N.Svirida, Z.W.Sweger, P.Szymanski, A.H.Tang, Z.Tang, A.Taranenko, T.Tarnowsky, J.H.Thomas, A.R.Timmins, D.Tlusty, T.Todoroki, M.Tokarev, C.A.Tomkiel, S.Trentalange, R.E.Tribble, P.Tribedy, S.K.Tripathy, T.Truhlar, B.A.Trzeciak, O.D.Tsai, Z.Tu, T.Ullrich, D.G.Underwood, I.Upsal, G.Van Buren, J.Vanek, A.N.Vasiliev, I.Vassiliev, V.Verkest, F.Videbaek, S.Vokal, S.A.Voloshin, F.Wang, G.Wang, J.S.Wang, P.Wang, Y.Wang, Y.Wang, Z.Wang, J.C.Webb, P.C.Weidenkaff, L.Wen, G.D.Westfall, H.Wieman, S.W.Wissink, J.Wu, Y.Wu, B.Xi, Z.G.Xiao, G.Xie, W.Xie, H.Xu, N.Xu, Q.H.Xu, Y.Xu, Z.Xu, Z.Xu, C.Yang, Q.Yang, S.Yang, Y.Yang, Z.Ye, Z.Ye, L.Yi, K.Yip, Y.Yu, H.Zbroszczyk, W.Zha, C.Zhang, D.Zhang, J.Zhang, S.Zhang, S.Zhang, X.P.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, Z.J.Zhang, Z.Zhang, Z.Zhang, J.Zhao, C.Zhou, X.Zhu, M.Zurek, M.Zyzak Global Λ-hyperon polarization in Au+Au collisions at √ sNN = 3 GeV
doi: 10.1103/PhysRevC.104.L061901
2021HU11 Phys.Rev. C 103, 044611 (2021) J.Hu, S.Wang, X.Sun, Y.Han, J.Zhang Model calculation of the differential cross sections and angle-integrated cross sections of the emitted triton for neutron-induced 6Li reactions at low incident energies NUCLEAR REACTIONS 6Li(n, t), E=1 eV-3 MeV; calculated differential and angle-integrated σ(E, θ) using Knock-out model based on zero-range DWBA theory, and Hauser-Feshbach model. Comparison with experimental and evaluated (JEFF-3.3 and ENDF/B-VIII-0) data.
doi: 10.1103/PhysRevC.103.044611
2021LI35 Eur.Phys.J. A 57, 232 (2021); Erratum Eur.Phys.J. A 57, 252 (2021) X.Liu, Y.Yang, R.Liu, Z.Wen, J.Wen, Z.Han, Y.Chen, H.Jing, H.Yi, J.Bao, Z.Ren, Q.An, H.Bai, P.Cao, Q.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, 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, 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 neutron total cross sections of aluminum at the back-n white neutron source of CSNS NUCLEAR REACTIONS 27Al(n, X), E<20 MeV; measured reaction products, En, In; deduced neutron transmission, total σ and uncertainties. Comparison withENDF/B-VIII.0, JEFF-3.3 and CENDL-3.2 library evaluations, EXFOR compilations. Spallation Neutron Source Science Center.
doi: 10.1140/epja/s10050-021-00513-9
2021RE01 Nucl.Instrum.Methods Phys.Res. A985, 164703 (2021) J.Ren, X.Ruan, W.Jiang, J.Bao, G.Luan, Q.Zhang, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, Z.Cui, R.Fan, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, Q.Mu, C.Ning, B.Qi, Z.Ren, Y.Song, Z.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Background study for (n, γ) cross section measurements with C6D6 detectors at CSNS Back-n NUCLEAR REACTIONS 197Au, Pb, C, 181Ta, 59Co(n, γ), E<400 MeV; measured reaction products, Eγ, Iγ; deduced σ.
doi: 10.1016/j.nima.2020.164703
2021SU09 Phys.Rev. C 103, 044603 (2021) Evolution of soft monopole mode in the even-even nickel isotopes 58-68Ni NUCLEAR STRUCTURE 58,60,62,64,66,68Ni; calculated centroid energies of soft isoscalar giant monopole resonances (ISGMR) for 68Ni, monopole strength functions for 58,60,62,64,66,68Ni, transition density for 68Ni, energy-weighted sum rule (EWSR) fraction; deduced that soft monopole mode dominated by neutron vibrations. Finite amplitude method (FAM) for covariant density functional theory (CDFT) with PC-PK1 functional for deformed nuclei. Comparison with available experimental data for monopole strength function and EWSR for 58Ni and 60Ni.
doi: 10.1103/PhysRevC.103.044603
2021SU10 Phys.Rev. C 103, 054315 (2021) Deformed two-neutron halo in 19B NUCLEAR STRUCTURE 19B; calculated S(2n), Fermi surfaces of neutrons, quadrupole deformation parameters β2, rms matter radii, proton and neutron density profiles, single neutron levels around the Fermi level, halo configurations and halo parameters. 15,17,19B; calculated angular averaged densities of neutrons, neutron halos and neutron cores. Deformed relativistic Hartree-Bogoliubov (DRHB) theory in continuum calculations using PC-PK1, PK1, NL3, DD-ME2, and PKDD density functionals.
doi: 10.1103/PhysRevC.103.054315
2021SU23 Phys.Rev. C 104, 064319 (2021) Angular momentum projection in the deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 38Mg; calculated total energy, rms matter radius, and quadrupole deformation parameter β2 of the ground state and oblate isomer. 24Mg; calculated normal overlap with the quadrupole deformation parameter, energies and B(E2) for the first 2+, 4+ and 6+ states. 36,38,40Mg; calculated ground-state properties, neutron, proton, and total quadrupole deformation parameters, neutron, proton, and total rms matter radii, the correction energies of center-of-mass spurious motion, the total energy, and the energies of the projected 0+ state, single-particle levels (SPLs) of neutrons around the Fermi energy, level energies, spectroscopic quadrupole moments, and B(E2) of the first 2+, 4+ and 6+ states of g.s. rotational bands. Angular momentum projection (AMP) method in the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc+AMP) with the point-coupling density functional PC-F1, with the wave functions of angular momentum projected states expanded in terms of the Dirac Woods-Saxon (WS) basis. Comparison with experimental values.
doi: 10.1103/PhysRevC.104.064319
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
2021YA02 Phys.Rev. C 103, 014304 (2021) S.Yang, X.D.Sun, J.Geng, B.Y.Sun, W.H.Long Liquid-gas phase transition of thermal nuclear matter and the in-medium balance between nuclear attraction and repulsion
doi: 10.1103/PhysRevC.103.014304
2021YA07 Phys.Rev.Lett. 126, 082501 (2021) Z.H.Yang, Y.Kubota, A.Corsi, K.Yoshida, X.-X.Sun, J.G.Li, M.Kimura, N.Michel, K.Ogata, C.X.Yuan, Q.Yuan, G.Authelet, H.Baba, C.Caesar, D.Calvet, A.Delbart, M.Dozono, J.Feng, F.Flavigny, J.-M.Gheller, J.Gibelin, A.Giganon, A.Gillibert, K.Hasegawa, T.Isobe, Y.Kanaya, S.Kawakami, D.Kim, Y.Kiyokawa, M.Kobayashi, N.Kobayashi, T.Kobayashi, Y.Kondo, Z.Korkulu, S.Koyama, V.Lapoux, Y.Maeda, F.M.Marques, T.Motobayashi, T.Miyazaki, T.Nakamura, N.Nakatsuka, Y.Nishio, A.Obertelli, A.Ohkura, N.A.Orr, S.Ota, H.Otsu, T.Ozaki, V.Panin, S.Paschalis, E.C.Pollacco, S.Reichert, J.-Y.Rousse, A.T.Saito, S.Sakaguchi, M.Sako, C.Santamaria, M.Sasano, H.Sato, M.Shikata, Y.Shimizu, Y.Shindo, L.Stuhl, T.Sumikama, Y.L.Sun, M.Tabata, Y.Togano, J.Tsubota, F.R.Xu, J.Yasuda, K.Yoneda, J.Zenihiro, S.-G.Zhou, W.Zuo, T.Uesaka Quasifree Neutron Knockout Reaction Reveals a Small s-Orbital Component in the Borromean Nucleus 17B NUCLEAR REACTIONS 1H(17B, np)16B, E ∼ 277 MeV/nucleon; measured reaction products, Eγ, Iγ. 17B; deduced energy levels, partial σ and spectroscopic parameters, resonance widths. Comparison with GSM, VS-IMSRG, AMD, SM calculations. MINOS target, RIKEN Nishina Center.
doi: 10.1103/PhysRevLett.126.082501
2021ZH24 Phys.Rev. C 103, 044314 (2021) H.B.Zhou, Z.G.Gan, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Li, C.X.Yuan, S.Huang, X.J.Sun, H.Y.Peng, L.Ou, X.H.Zhou Lifetime measurement for the isomeric state in 213Th NUCLEAR REACTIONS 176Hf(40Ar, xn)213Th/214Th/215Th, E=183, 190 MeV beam from Sector-Focusing Cyclotron of HIRFL-Lanzhou facility, followed by the separation of evaporation residues (ERs) by the SHANS separator and implanted in three position-sensitive silicon strip detectors (PSSDs); measured position, time, and energy of the ERs, Eα, Iα, Eγ, Iγ, (ER)α-, (ER)γ- and (ER)αγ-correlated events. Enriched target. 213,214,215Th; deduced levels, J, π, isomers, half-lives of the isomers in 213,214,215Th. Comparison with previous experimental results for isomer half-lives. Systematics of 13/2+ isomers in N=123 isotones 207Po, 209Rn, 211Ra and 213Th. RADIOACTIVITY 209,210,211,213Ra, 212,213,215Ac, 211,212,213,214,215,216Th(α)[from 176,177,178,179,180Hf(40Ar, xnyp), E=183, 190 MeV, enriched 176Hf with small abundance of other Hf isotopes]; measured Eα, Iα, αγ-correlations.
doi: 10.1103/PhysRevC.103.044314
2020BA03 Chin.Phys.C 44, 014003 (2020) H.Bai, R.Fan, H.Jiang, Z.Cui, Y.Hu, G.Zhang, Z.Chen, W.Jiang, H.Yi, J.Tang, L.Zhou, Q.An, J.Bao, P.Cao, Q.Chen, Y.Chen, P.Cheng, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.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, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the differential cross sections and angle-integrated cross sections of the 6Li(n, t)4He reaction from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), E=0.000001-3 MeV; measured reaction products; deduced σ. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries, experimental data.
doi: 10.1088/1674-1137/44/1/014003
2020DU02 Chin.Phys.C 44, 024001 (2020) F.-F.Duan, Y.-Y.Yang, D.-Y.Pang, B.-T.Hu, J.-S.Wang, K.Wang, G.Yang, V.Guimaraes, P.Ma, S.-W.Xu, X.-Q.Liu, J.-B.Ma, Z.Bai, Q.Hu, S.-Y.Jin, X.-X.Sun, J.-S.Yao, H.-K.Qi, Z.-Y.Sun Experimental study of the elastic scattering of 10Be on 208Pb at the energy of around three times the Coulomb barrier NUCLEAR REACTIONS 208Pb(8Be, 8Be), E=127 MeV; measured reaction products; deduced σ, optical model parameters.
doi: 10.1088/1674-1137/44/2/024001
2020DU18 Phys.Lett. B 811, 135942 (2020) F.F.Duan, Y.Y.Yang, K.Wang, A.M.Moro, V.Guimaraes, D.Y.Pang, J.S.Wang, Z.Y.Sun, J.Lei, A.Di Pietro, X.Liu, G.Yang, J.B.Ma, P.Ma, S.W.Xu, Z.Bai, X.X.Sun, Q.Hu, J.L.Lou, X.X.Xu, H.X.Li, S.Y.Jin, H.J.Ong, Q.Liu, J.S.Yao, H.K.Qi, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu Scattering of the halo nucleus 11Be from a lead target at 3.5 times the Coulomb barrier energy NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, X), E=140 MeV; 208Pb(10Be, X), (10Be, X), E=127 MeV; 208Pb(9Be, 9Be), (9Be, X), E=88 MeV; measured reaction products. 9,10,11Be; deduced σ(θ), σ(E), σ. Comparison with continuum discretized coupled channel (CDCC) as well as by the XCDCC calculations.
doi: 10.1016/j.physletb.2020.135942
2020GA34 J.Phys.(London) G47, 045108 (2020) J.Galan, X.Chen, H.Du, C.Fu, K.Giboni, F.Giuliani, K.Han, B.Jiang, X.Ji, H.Lin, Y.Lin, J.Liu, K.Ni, X.Ren, S.Wang, S.Wu, C.Xie, Y.Yang, T.Zhang, L.Zhao, S.Aune, Y.Bedfer, E.Berthoumieux, D.Calvet, N.d'Hose, E.Ferrer-Ribas, F.Kunne, B.Manier, D.Neyret, T.Papaevangelou, L.Chen, S.Hu, P.Li, X.Li, H.Zhang, M.Zhao, J.Zhou, Y.Mao, H.Qiao, S.Wang, Y.Yuan, M.Wang, Y.Chen, A.N.Khan, J.Tang, W.Wang, H.Chen, C.Feng, J.Liu, S.Liu, X.Wang, D.Zhu, J.F.Castel, S.Cebrian, T.Dafni, I.G.Irastorza, G.Luzon, H.Mirallas, X.Sun, A.Tan, W.Haxton, Y.Mei, C.Kobdaj, Y.Yan Topological background discrimination in the PandaX-III neutrinoless double beta decay experiment
doi: 10.1088/1361-6471/ab4dbe
2020HU05 Phys.Rev. C 101, 034616 (2020) J.Hu, X.Sun, J.Zhang, S.Wang, Y.Han Theoretical analysis of double-differential cross sections of proton, deuteron, and triton emission in thee p + 7Li reaction at 14 MeV NUCLEAR REACTIONS 7Li(p, p'), (p, d), (p, t), (p, pd), (p, pt), (p, 2d), (p, 3He), (p, α), (p, pα), (p, dα), (p, 5He), E=14 MeV; calculated double differential σ(θ) using statistical theory of light nucleus reactions (STLN), including the sequential and simultaneous emission processes. Comparison with available experimental data.
doi: 10.1103/PhysRevC.101.034616
2020JI04 Phys.Rev. C 101, 031304 (2020) W.Jiang, Y.L.Ye, C.J.Lin, Z.H.Li, J.L.Lou, X.F.Yang, Q.T.Li, Y.C.Ge, H.Hua, D.X.Jiang, D.Y.Pang, J.Li, J.Chen, Z.H.Yang, X.H.Sun, Z.Y.Tian, J.Feng, B.Yang, H.L.Zang, Q.Liu, P.J.Li, Z.Q.Chen, Y.Liu, Y.Zhang, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun Determination of the cluster-decay branching ratio from a near-threshold molecular state in 10Be NUCLEAR REACTIONS 9Be(9Be, 10Be)8Be, E=45 MeV; measured Eα, Iα, E(6He), I(6He), E(9Be), I(9Be), α(6He)-coin, and σ of 10Be population channel from the decay of 10Be* to α+6He using ΔE-E telescope detectors at CIAE HI-13 tandem accelerator facility. 10Be; deduced Q-value spectra, resonances, α-decay branching ratio, and α-cluster spectroscopic factor, σ-bond molecular rotational band. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.101.031304
2020JI06 Nucl.Instrum.Methods Phys.Res. A973, 164126 (2020) W.Jiang, H.Bai, H.Jiang, H.Yi, R.Fan, G.Zhang, J.Tang, Z.Sun, C.Ning, K.Sun, K.Gao, Z.Cui, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Y.Song, Z.Song, H.Sun, X.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Application of a silicon detector array in (n, lcp) reaction cross-section measurements at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), 10B(n, α), E<1 MeV; measured reaction products, En, In; deduced σ. Comparison with experimental data, ENDF/B-VIII.0, JEFF-3.3, ROSFOND evaluated libraries.
doi: 10.1016/j.nima.2020.164126
2020LI14 Phys.Rev.Lett. 124, 192501 (2020) Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, J.X.Han, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song Positive-Parity Linear-Chain Molecular Band in 16C NUCLEAR REACTIONS 2H(16C, X)2H, E=23.5 MeV/nucleon; measured reaction products, Eα, Iα. 16C; deduced excitation energies, spin parities, total decay widths of the resonances in 16C. Comparison with AMD calculations.
doi: 10.1103/PhysRevLett.124.192501
2020LI33 Nucl.Instrum.Methods Phys.Res. A980, 164506 (2020) Q.Li, H.Jing, B.Zhou, C.Ning, J.Tang, J.Ren, H.Yi, X.Zhu, L.Zhang, W.Jiang, R.Fan, J.Bao, C.Feng, X.Ruan, Y.Chen, L.Zhou, Y.Li, Z.Tan, Y.Chen, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, L.Kang, M.Kang, B.Li, L.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, B.Qi, Z.Song, H.Sun, X.Sun, Z.Sun, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, J.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 Neutron and γ background measurements of the experimental halls at the CSNS back-streaming white neutron source
doi: 10.1016/j.nima.2020.164506
2020LI51 Phys.Rev. C 102, 064601 (2020) J.J.Li, C.A.Bertulani, Y.Liu, J.L.Lou, D.Y.Pang, X.H.Sun, B.Yang, X.F.Yang, Y.L.Ye Eikonal method for charge-exchange reactions at intermediate energies NUCLEAR REACTIONS 26Mg, 120Sn(3He, t), E=140 MeV/nucleon; 13C(13N, 13C), E=105 MeV/nucleon; calculated differential σ(θ) and relativistic kinematical quantities for intermediate and high energy heavy-ion charge exchange reactions using Eikonal method and the DWBA model, with effective nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.064601
2020RE09 Phys.Rev. C 101, 064905 (2020) K.Reygers, A.Schmah, A.Berdnikova, X.Sun Blast-wave description of Υ elliptic flow at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.101.064905
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
2020SU07 Phys.Rev. C 101, 034302 (2020) X.Sun, R.Xu, Y.Tian, Z.Ma, Z.Zhang, Z.Ge, H.Zhang, E.N.E.van Dalen, H.Muther Relativistic mean-field approach in nuclear systems NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,132Sn, 208Pb; calculated binding energy per nucleon, charge radii, charge density distribution, single particle energies, spin-orbit splitting in 16O, scalar and vector potentials for neutrons and protons as a function of isospin asymmetry using both local density approximation (LDA) and improved LDA, based on Dirac-Brueckner-Hartree-Fock (DBHF) approach starting from a realistic nucleon-nucleon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.034302
2020SU09 Phys.Rev. C 101, 035503 (2020) X.Sun, for the UCNA Collaboration Improved limits on Fierz interference using asymmetry measurements from the Ultracold Neutron Asymmetry (UCNA) experiment RADIOACTIVITY 1n(β-); measured decay asymmetry and energy spectrum distortion of polarized ultracold neutrons (UCNs) at LANSCE of LANL facility (UCNA Collaboration); deduced Fierz interference term of neutron β- decay at 90% confidence limits.
doi: 10.1103/PhysRevC.101.035503
2020SU16 Phys.Rev. C 101, 064623 (2020) X.H.Sun, H.Wang, H.Otsu, H.Sakurai, D.S.Ahn, M.Aikawa, N.Fukuda, T.Isobe, S.Kawakami, S.Koyama, T.Kubo, S.Kubono, G.Lorusso, Y.Maeda, A.Makinaga, S.Momiyama, K.Nakano, S.Nakayama, M.Niikura, Y.Shiga, P.-A.Soderstrom, H.Suzuki, H.Takeda, S.Takeuchi, R.Taniuchi, Ya.Watanabe, Yu.Watanabe, H.Yamasaki, X.F.Yang, Y.L.Ye, K.Yoshida Spallation and fragmentation cross sections for 168 MeV/nucleon 136Xe ions on proton, deuteron, and carbon targets NUCLEAR REACTIONS 1,2H, C(136Xe, X), E=168 MeV/nucleon, 89Zr/90Zr/91Zr/92Zr/93Zr/94Zr/91Nb/92Nb/93Nb/94Nb/95Nb/96Nb/93Mo/94Mo/95Mo/96Mo/97Mo/98Mo/99Mo/96Tc/97Tc/98Tc/99Tc/100Tc/101Tc/102Tc/97Ru/98Ru/99Ru/100Ru/101Ru/102Ru/103Ru/104Ru/105Ru/106Ru/99Rh/100Rh/101Rh/102Rh/103Rh/104Rh/105Rh/106Rh/107Rh/108Rh/102Pd/103Pd/104Pd/105Pd/106Pd/107Pd/108Pd/109Pd/110Pd/104Ag/105Ag/106Ag/107Ag/108Ag/109Ag/110Ag/111Ag/112Ag/113Ag/114Ag/107Cd/108Cd/109Cd/110Cd/111Cd/112Cd/113Cd/114Cd/115Cd/116Cd/109In/110In/111In/112In/113In/114In/115In/116In/117In/118In/119In/111Sn/112Sn/113Sn/114Sn/115Sn/116Sn/117Sn/118Sn/119Sn/120Sn/121Sn/122Sn/113Sb/114Sb/115Sb/116Sb/117Sb/118Sb/119Sb/120Sb/121Sb/122Sb/123Sb/124Sb/125Sb/116Te/117Te/118Te/119Te/120Te/121Te/122Te/123Te/124Te/125Te/126Te/127Te/128Te/129Te/130Te/131Te/132Te/133Te/134Te/118I/119I/120I/121I/122I/123I/124I/125I/126I/127I/128I/129I/130I/131I/132I/133I/134I/135I/121Xe/122Xe/123Xe/124Xe/125Xe/126Xe/127Xe/128Xe/129Xe/130Xe/131Xe/132Xe/133Xe/134Xe/135Xe/123Cs/124Cs/125Cs/126Cs/127Cs/128Cs/129Cs/130Cs/131Cs/132Cs/133Cs/134Cs/135Cs/136Cs, [secondary 136Xe beam from 9Be(238U, F), E=345 MeV/nucleon primary reaction]; measured reaction products using the BigRIPS separator and ZeroDegree spectrometer at RIBF-RIKEN facility; deduced isotopic production σ and total σ by analyzing the data using the Particle and Heavy Ion Transport code System (PHITS) including dynamical and intranuclear cascade processes and evaporation process, the semi-empirical parametrization for residue cross sections in spallation reactions (SPACS), empirical parametrization of fragmentation cross sections (EPAX), and the deuteron-induced reaction analysis code system (DEURACS) incorporating the deuteron breakup effect. Comparison with theoretical calculations using the JQMD+GEM and INCL+GEM codes.
doi: 10.1103/PhysRevC.101.064623
2020SU20 Nucl.Phys. A1003, 122011 (2020) Study of ground state properties of carbon isotopes with deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 12,13,14,15,16,17,18,19,20,21,22C; analyzed available data; calculated neutron separation energies, rms matter radii, deformation parameters.
doi: 10.1016/j.nuclphysa.2020.122011
2020WE04 Ann.Nucl.Energy 140, 107301 (2020) J.Wen, Y.Yang, Z.Wen, R.Liu, X.Liu, Z.Han, Q.Chen, Z.Ren, 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 U-238/U-235 fission cross section ratio at CSNS - Back-in WNS NUCLEAR REACTIONS 235,238U(n, F), E=1-20 MeV; measured reaction products, fission fragments, Eγ, Iγ; deduced neutron resonances, σ. Comparison with ENDF/B-VIII.0 library evaluations.
doi: 10.1016/j.anucene.2019.107301
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
2019CH37 Eur.Phys.J. A 55, 115 (2019), Erratum Eur.Phys.J. A 55, 145 (2019) Y.Chen, G.Luan, J.Bao, H.Jing, L.Zhang, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, Ch.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, 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, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.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 Neutron energy spectrum measurement of the Back-n white neutron source at CSNS
doi: 10.1140/epja/i2019-12808-1
2019JI07 Chin.Phys.C 43, 124002 (2019) H.Jiang, W.Jiang, H.Bai, Z.Cui, G.Zhang, R.Fan, H.Yi, C.Ning, L.Zhou, J.Tang, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Z.Song, Y.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurements of differential and angle-integrated cross sections for the 10B(n, α)7Li reaction in the neutron energy range from 1.0 eV to 2.5 MeV NUCLEAR REACTIONS 10B(n, α), E=0.000001-2.5 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ and uncertainties. Comparison with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1 and JENDL 4.0 libraries.
doi: 10.1088/1674-1137/43/12/124002
2019SU11 Phys.Rev. C 99, 054604 (2019) Neutron-proton mass splitting and pygmy dipole resonance in 208Pb NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated binding energies, charge radii, nuclear density, and other bulk properties of the nuclear matter. Comparison with experimental values. 48Ca, 208Pb; calculated neutron skin thicknesses, transition strength distribution of the electric dipole resonance, centroid energies of the giant dipole resonance (GDR) and pygmy dipole resonances (PDR). Comparison with experimental data. 208Pb; calculated dominating excited states in the pygmy dipole resonance of with the inclusion of δ meson, symmetry energy, relationship between the neutron-proton effective mass splitting and the difference of the centroid energies of GDR and PDR. Random phase approximation method, with the effect of the neutron-proton mass splitting treated in the framework of relativistic mean field theory by including the scalar-isovector meson δ explicitly.
doi: 10.1103/PhysRevC.99.054604
2019SU24 Chin.Phys.Lett. 38, 112501 (2019) X.-J.Sun, F.-Q.Zhou, Y.-L.Song, Y.Li, P.-F.Ji, X.-Y.Chang Measurements of the Cross-sections of Produced Short-Lived Nuclei Induced by Neutrons around 14 MeV on Isotopes of Tungsten* NUCLEAR REACTIONS 180,186W(n, 2n), 186W(n, p), E=13.5, 14.4 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data.
doi: 10.1088/0256-307X/36/11/112501
2019SU26 Phys.Rev. C 100, 054605 (2019) Effects of the γ-soft isomeric states on the giant monopole resonances in even-even cadmium isotopes 110, 112, 114, 116Cd NUCLEAR STRUCTURE 110,112,114,116Cd; calculated potential energy surfaces in (β, γ) plane, strength functions of giant monopole resonances (GMRs), β and γ deformation parameters, centroid energies of the GMRs built on isomeric states in the Cd isotopes. Discussed contribution of shape isomer mixing to the GMR strength in an excited nucleus. Quasiparticle random phase approximation (QRPA), implemented with a finite amplitude method. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.054605
2019ZH30 Nucl.Instrum.Methods Phys.Res. B451, 24 (2019) F.Zhou, Y.Song, Y.Li, X.Sun, X.Chang Measurements of fast neutron capture cross section for 180Hf NUCLEAR REACTIONS 180Hf(n, γ), E ∼ 14 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS-1.8 nuclear model code calculations.
doi: 10.1016/j.nimb.2019.04.084
2019ZH39 Nucl.Phys. A990, 1 (2019) Z.Zhang, R.R.Xu, Z.Y.Ma, Z.G.Ge, Y.Tian, D.Y.Pang, X.D.Sun, Y.L.Jin, X.Tao, Y.Zhang, J.M.Wang Global α-nucleus optical model based on an Dirac Brueckner Hartree Fock approach
doi: 10.1016/j.nuclphysa.2019.06.013
2019ZH40 Chin.Phys.C 43, 094001 (2019) F.Zhou, Y.Song, Y.Li, X.Sun, S.Yuan Activation cross-sections of titanium isotopes at neutron energies of 13.5-14.8 MeV NUCLEAR REACTIONS 46Ti(n, 2n), (n, p), 47Ti(n, d), (n, p), 48Ti(n, d), (n, p), 49Ti(n, d), 50Ti(n, α), E=13.5–14.8 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with JEFF-3.3, CENDL-3.1, ENDF/B-VIII.0 libraries, as well as results calculated by Talys-1.9 code.
doi: 10.1088/1674-1137/43/9/094001
2018CH08 Phys.Rev. C 97, 025802 (2018) G.Christian, G.Lotay, C.Ruiz, C.Akers, D.S.Burke, W.N.Catford, A.A.Chen, D.Connolly, B.Davids, J.Fallis, U.Hager, D.Hutcheon, A.Mahl, A.Rojas, X.Sun Direct measurement of astrophysically important resonances in 38K(p, γ) 39Ca NUCLEAR REACTIONS 1H(38K, γ)39Ca, E=15.58, 20.56, 27.17 MeV, [38K secondary beam produced at ISAC-I, TRIUMF facility by impinging 500 MeV protons on a high-power TiC production target]; measured recoils using DRAGON spectrometer, prompt Eγ, Iγ, (recoil)γ-coin using bismuth-germanate scintillator array for γ detection. Windowless hydrogen gas target; deduced energies of resonances, resonance strengths for the 386-, 515- and 689-keV proton resonances, astrophysical reaction rates for temperature range of 150-500 MK, abundances of 38Ar, 39K, and 40Ca in the hottest oxygen-neon novae.
doi: 10.1103/PhysRevC.97.025802
2018SU01 Chin.Phys.C 42, 014101 (2018) Stagnancy of the pygmy dipole resonance NUCLEAR STRUCTURE 58,60,62,64,66,68,70,72,74,76,78Ni; calculated pygmy dipole resonance (PDR) parameters of nickel isotopes using the deformed random phase approximation; deduced a linear correlation between PDR integral σ and neutron skin thickness when the excess neutrons lie in pf orbits.
doi: 10.1088/1674-1137/42/1/014101
2018SU06 Phys.Rev. C 97, 052501 (2018) X.Sun, for the UCNA Collaboration Search for dark matter decay of the free neutron from the UCNA experiment: n → x + e+e- RADIOACTIVITY 1n(β-); analyzed β-decay data from polarized Ultracold Neutrons (UCNs) at LANSCE-LANL facility; deduced rate of electron-positron pair production, and limits on theoretical neutron dark decay channel. Relevance to discrepancy in the neutron lifetime measured in experiments using two different techniques.
doi: 10.1103/PhysRevC.97.052501
2018SU09 J.Phys.(London) G45, 075106 (2018) α decay preformation probabilities across the N = 126 shell closure based on the single particle energy spectra RADIOACTIVITY 192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226Ra, 214,216,218,220,222,224,226,228,230,232Th(α); calculated partial neutron and proton single particle energy spectra, microscopic valence neutron (hole) and proton numbers, α decay preformation probabilities, T1/2, quadrupole deformation parameters. The relativistic Hartree-Bogoliubov model.
doi: 10.1088/1361-6471/aac981
2018SU18 Phys.Rev. C 98, 024607 (2018) Pygmy dipole resonance built on the shape-isomeric state in 68Ni NUCLEAR REACTIONS 68Ni(γ, X), E*=7-35 MeV; calculated virtual γ photoabsorption σ for spherical ground state and prolate isomeric state of 68Ni using deformed relativistic random phase approximation method. 68Ni; calculated potential energy surface (PES) contour in (β, γ) plane, radial distributions of dominant states contributing to pygmy dipole resonance (PDR) and giant dipole resonance (GDR), pygmy dipole resonance energy of spherical ground state and prolate isomeric state; deduced effect of the shape-coexistence isomeric state in 68Ni. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.024607
2018SU22 Phys.Lett. B 785, 530 (2018) Shrunk halo and quenched shell gap at N=16 in 22C: Inversion of sd states and deformation effects NUCLEAR STRUCTURE 22C; analyzed available data; deduced inversion between the two spherical orbitals, shrunk halo and a quenched shell gap at N=16.
doi: 10.1016/j.physletb.2018.08.071
2018SU24 Chin.Phys.C 42, 124105 (2018) X.-J.Sun, C.-X.Chen, N.Wang, H.-B.Zhou Systematic description of nuclear electric quadrupole moments NUCLEAR STRUCTURE A=2-260; calculated nuclear electric quadrupole moments. Comparison with available data.
doi: 10.1088/1674-1137/42/12/124105
2017LI04 Phys.Rev. C 95, 021303 (2017) J.Li, Y.L.Ye, Z.H.Li, C.J.Lin, Q.T.Li, Y.C.Ge, J.L.Lou, Z.Y.Tian, W.Jiang, Z.H.Yang, J.Feng, P.J.Li, J.Chen, Q.Liu, H.L.Zang, B.Yang, Y.Zhang, Z.Q.Chen, Y.Liu, X.H.Sun, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun Selective decay from a candidate of the σ-bond linear-chain state in 14C NUCLEAR REACTIONS 9Be(9Be, α10Be)He, E=45 MeV; measured particle spectra at HI-13 tandem accelerator of CIAE-Beijing facility. 14C; deduced level energies from reconstruction of forward moving 10Be+α fragments, resonances, decays to α cluster and 10Be in its ground state, first 2+, and about 6-MeV state, relative decay strength, indication of a σ-bond linear chain structure in 14C. Comparison with predictions of improved antisymmetrized molecular dynamics (AMD) theory.
doi: 10.1103/PhysRevC.95.021303
2017SU02 Chin.Phys.C 41, 014102 (2017) X.-D.Sun, X.-J.Wu, B.Zheng, D.Xiang, P.Guo, X.-H.Li Systematic study of α preformation probability of nuclear isomeric and ground states RADIOACTIVITY 177,175,173Au, 173,171,169,167Ir, 169,167,163Re, 177Tl, 159Ta, 155Lu, 153,151Ho, 149Tb, 153Tm, 185Hg, 185,187,189,191Pb, 195,197,199,201,203Po, 195,197,203Rn, 203,209Ra, 187,189,191,193,195,197Bi, 191,193,197At, 201Fr(α); calculated T1/2 and the α-particle preformation probabilities. Comparison with available data.
doi: 10.1088/1674-1137/41/1/014102
2017SU06 Phys.Rev. C 95, 014319 (2017) X.-D.Sun, C.Duan, J.-G.Deng, P.Guo, X.-H.Li Systematic study of α decay for odd-A nuclei within a two-potential approach RADIOACTIVITY 145Pm, 147Sm, 147Eu, 149Gd, 149,149m,151Tb, 151,153Dy, 151,151m,153,153mHo, 153,155Er, 153,153m,155Tm, 155,157Yb, 155,155m,157mLu, 157Hf, 159,159mTa, 159,161,163W, 159m,161m,163,163m,165m,167m,169mRe, 161,163,165,167,169Os, 165m,167,167m,169,169m,171m,173m,175,177Ir, 167,171,173,175,177,179,181,183Pt, 173,175,177,179,181,183,185Au, 173,177,179,183,185Hg, 177,183,187mTl, 179,185,185m,187,187m,189,191mPb, 185m,187m,189m,191m,193m,195m,209,211,213Bi, 187,189,195,195m,197,199,201,203,205,207,211,213,215,217Po, 191m,193m,197,199,201,203,205,207,209,211,213,215,217At, 193,195,195m,197,203,205,207,209,213,215,217,219,221,223Rn, 199,201,203,205,207,209,211,213,215,219,221,223Fr, 203,207,209,211,213,215,217,219,221,223Ra, 207,211,215,217,219,221,223,225,227Ac, 215,217,219,221,223,225,227,229,231Th, 213,215,217,217m,219,221,223,227,229,231Pa, 219,225,227,229,231,235U, 225,227,229,231,235,237,239Np, 229,231,233,235,237,241Pu, 233,235,237,239,241,243Am, 233,237,239,243,245,247Cm, 243,245,247,249Bk, 247,249,255Cf, 243,251,253Es, 243,247,247m,251,255,257Fm, 247,247m,251,253,255,257Md, 251No, 253,255mLr, 255m,257m,261,263Rf, 257Db, 259m,261,263,265Sg, 265,267Hs, 267,269,271,271m,273,273m,277,281Ds, 281,285Cn, 289Fl(α); calculated α-decay half-lives for odd-A nuclei, preformation probabilities, and compared with experimental values. Two-potential approach based on isospin dependent nuclear potential.
doi: 10.1103/PhysRevC.95.014319
2017SU11 Phys.Rev. C 95, 044303 (2017) X.-D.Sun, J.-G.Deng, D.Xiang, P.Guo, X.-H.Li Systematic study of α decay half-lives of doubly odd nuclei within the two-potential approach RADIOACTIVITY 105,106,107,108,109,110Te, 108,109,110,111,112,113I, 109,110,111,112,113,115Xe, 112,114Cs, 114Ba, 148Eu, 152,154Ho, 154,156Tm, 156Lu, 158Ta, 160,162,164,166Re, 166,168,170,172,174Ir, 170,186Au, 180,186Tl, 190,192,194,196,212,214Bi, 192,194,198,200,202,204,206,208,210,212,214,216,218At, 202,204,208,210,212,214,216,218,220Fr, 212,220,224,228Pa, 214,216,218,220,222,226Ac, 232,236Np, 236,238,242Am, 246,248Bk, 244,246,248,252,254Es, 246,248,250,256,258,260Md, 254,258,260Lr, 272,274,278,280,282Rg, 258,260,262,268Db, 260,264,266,270,272,274Bh, 268,270,274,276,278Mt, 278,282,284,286Nh, 288,290Mc, 292,294Ts, 296119(α); calculated α-decay half-lives, and α preformation probabilities for odd-odd nuclei using a two-potential approach, and compared with experimental values.
doi: 10.1103/PhysRevC.95.044303
2017SU24 Phys.Rev. C 96, 024614 (2017) Implementation of a finite-amplitude method in a relativistic meson-exchange model NUCLEAR STRUCTURE 110,112,114,116Cd, 208Pb; calculated isoscalar giant monopole resonance (ISGMR) strength distributions, and compared with available experimental data. 60Ni; calculated electric dipole resonance strength distribution. Finite-amplitude method (FMA) and large scale random phase approximation (RPA) calculations.
doi: 10.1103/PhysRevC.96.024614
2016FA10 Phys.Rev. C 94, 044621 (2016) D.Q.Fang, Y.G.Ma, X.Y.Sun, P.Zhou, Y.Togano, N.Aoi, H.Baba, X.Z.Cai, X.G.Cao, J.G.Chen, Y.Fu, W.Guo, Y.Hara, T.Honda, Z.G.Hu, K.Ieki, Y.Ishibashi, Y.Ito, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Ooishi, K.Okada, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, W.D.Tian, H.W.Wang, J.S.Wang, M.Wang, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, G.Q.Zhang, T.Motobayashi Proton-proton correlations in distinguishing the two-proton emission mechanism of 23Al and 22Mg NUCLEAR REACTIONS 12C(23Al, 2pX), (23Al, 2p21Na), (23Al, 2p20Ne), E=57.4 MeV/nucleon; 12C(22Mg, 2pX), (22Mg, 2p20Ne), E=53.5 MeV/nucleon, [secondary 22Mg and 23Al beams from 12C(28Si, X), E=135 MeV/nucleon primary reaction]; measured fragments and protons using ΔE-E detectors at RIBF-RIKEN facility; deduced proton-proton momentum correlation function for decays into p+p+X, p+p+20Na, and p+p+21Na channels, effective source sizes from calculations using the CRAB code with a Gaussian source, mechanism of two-proton emission.
doi: 10.1103/PhysRevC.94.044621
2016LO03 Phys.Rev.Lett. 116, 132701 (2016) G.Lotay, G.Christian, C.Ruiz, C.Akers, D.S.Burke, W.N.Catford, A.A.Chen, D.Connolly, B.Davids, J.Fallis, U.Hager, D.A.Hutcheon, A.Mahl, A.Rojas, X.Sun Direct Measurement of the Astrophysical 38K(p, γ)39Ca Reaction and Its Influence on the Production of Nuclides toward the End Point of Nova Nucleosynthesis NUCLEAR REACTIONS 1H(38K, γ), E=386, 515, 689 keV; measured reaction products, Eγ, Iγ; deduced yields, resonance parameters, astrophysical reaction rates. Comparison with available data.
doi: 10.1103/PhysRevLett.116.132701
2016SU04 Phys.Rev. C 93, 014609 (2016) Statistical theory of light-nucleus reactions and application to the 9Be(p, xn) reaction NUCLEAR REACTIONS 9Be(p, n), (p, np), (p, pα), (p, xn), E=18 MeV; calculated partial double-differential cross sections, σ(θ), total double-differential cross sections for (p, xn) as function of outgoing neutron energy. Comparison with experimental data. Statistical theory of light nucleus reactions (STLN).
doi: 10.1103/PhysRevC.93.014609
2016SU09 Phys.Rev. C 93, 034316 (2016) Systematic study of α decay half-lives for even-even nuclei within a two-potential approach RADIOACTIVITY 146Sm, 148,150Gd, 150,152,154Dy, 152,154,156Er, 154,156,158Yb, 156,158,160,162Hf, 158,160,162,164,166,168W, 166,168,170,172,174,186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt, 172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194,210Pb, 190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226Ra, 214,216,218,220,222,224,226,228,230,232Th, 224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248,250Cm, 240,242,244,246,248,250,252,254Cf, 248,250,252,254,256Fm, 252,254,256No, 254,256,258Rf, 260,266Sg, 264,266Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α); calculated half-lives for α decay of Z=62-118 even-even nuclei using two-potential approach based on isospin-dependent nuclear potential taking into account hindrance factors; deduced parameters of isospin-dependent nuclear potentials and analytic expression of hindrance factors. Comparison with experimental half-lives, and with results from density-dependent cluster model (DDCM) and the generalized liquid drop model (GLDM).
doi: 10.1103/PhysRevC.93.034316
2016SU19 Phys.Rev. C 94, 024338 (2016) Systematic study of favored α-decay half-lives of closed shell odd-A and doubly-odd nuclei related to ground and isomeric states RADIOACTIVITY 151Dy, 151,151mHo, 153Er, 153,153m,154,154m,155Tm, 155,157Yb, 155,155m,156m,157mLu, 157Hf, 158,158m,159,159mTa, 159,161,163W, 159m,161m,162m,162m,163,163m,165mRe, 161,163,165,167,169Os, 165m,166,166m,167,167m,169,169mIr, 167,171,173Pt, 170,170m,173,175,177Au, 177,183Tl, 179,183Hg, 185m,187m,191mPb, 187m,189m,191m,193m,195mBi, 195,195m,197,199,201,205,207Po, 197,198,199,200,201,202,203,204,205,206,207,208,209,211,214,214m,218At, 203,207,209,215,217Rn, 204,205,207,208,209,211,213,215,216,216m,217,218,219Fr, 209,211,217Ra, 213,215,217,219,220,221Pa, 211,213,217,218,219Ac, 219Th(α); calculated half-lives for favored α decays of ground and isomeric states of closed shell odd-A and doubly-odd nuclei using the semiclassical WKB method with the isospin dependent nuclear potential; evaluated α preformation probabilities by the linear relationships of NpNn and NpNnI, where I=asymmetry parameter between neutrons and protons in parent nuclei. Comparison with experimental data taken from NUBASE-2012.
doi: 10.1103/PhysRevC.94.024338
2016TI10 Chin.Phys.C 40, 111001 (2016) Z.Y.Tian, Y.L.Ye, Z.H.Li, C.J.Lin, Q.T.Li, Y.C.Ge, J.L.Lou, W.Jiang, J.Li, Z.H.Yang, J.Feng, P.J.Li, J.Chen, Q.Liu, H.L.Zang, B.Yang, Y.Zhang, Z.Q.Chen, Y.Liu, X.H.Sun, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun Cluster decay of the high-lying excited states in 14C NUCLEAR REACTIONS 9Be(9Be, 14C), E=45 MeV; measured reaction products, Eα, Iα. 14C, 10Be; deduced low-lying resonance states, cluster structures.
doi: 10.1088/1674-1137/40/11/111001
2015MA19 Phys.Lett. B 743, 306 (2015) Y.G.Ma, D.Q.Fang, X.Y.Sun, P.Zhou, Y.Togano, N.Aoi, H.Baba, X.Z.Cai, X.G.Cao, J.G.Chen, Y.Fu, W.Guo, Y.Hara, T.Honda, Z.G.Hu, K.Ieki, Y.Ishibashi, Y.Ito, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Ooishi, K.Okada, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, W.D.Tian, H.W.Wang, J.S.Wang, M.Wang, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, G.Q.Zhang, T.Motobayashi Different mechanism of two-proton emission from proton-rich nuclei 23Al and 22Mg RADIOACTIVITY 23Al, 22Mg(2p) [from 9Be(28Si, X), E=135 MeV/nucleon]; measured decay products, Ep, Ip; deduced two-proton relative momentum and opening angle from the decay. Comparison with available data.
doi: 10.1016/j.physletb.2015.02.066
2015SU02 Chin.Phys.C 39, 014102 (2015) X.-J.Sun, C.-G.Yu, N.Wang, Y.-X.Yang, C.H.Pan Pre-neutron-emission mass distributions for reaction 238U(n, f) up to 60 MeV NUCLEAR REACTIONS 238U(n, F), E<60 MeV; analyzed available data; deduced σ, preneutron-emission mass distributions, fission yields. Empirical fission potential model, comparison with available data.
doi: 10.1088/1674-1137/39/1/014102
2015SU05 Phys.Rev. C 91, 024903 (2015) X.Sun, H.Masui, A.M.Poskanzer, A.Schmah Blast wave fits to elliptic flow data at √ sNN = 7.7-2760 GeV
doi: 10.1103/PhysRevC.91.024903
2015SU13 Phys.Rev. C 92, 061601 (2015) New integral formula for obtaining analytical Legendre expansion coefficients and its applications to light-nucleus reactions NUCLEAR REACTIONS 9Be(p, n), (p, np), (p, pα), (p, 5He), E=18 MeV; calculated partial and total energy-angular spectra using a newly developed integral formula under the general framework of statistical theory of light nucleus (STLN) reactions. Sequential emission process, neutron double-differential cross section. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.061601
2015ZH40 Chin.Phys.C 39, 114103 (2015) H.-B.Zhou, G.-X.Dong, X.-J.Sun, F.-R.Xu Phase transition in odd-N Pd-isotopes NUCLEAR STRUCTURE 99,101,103Pd; calculated total Routhian surfaces for the lowest configurations, quasiproton and quasineutron Routhians as a function of the rotational frequency. The framework of the cranked shell model (CSM), comparison with experimental data.
doi: 10.1088/1674-1137/39/11/114103
2014WA31 Nucl.Data Sheets 120, 6 (2014) M.Wang, G.Audi, F.G.Kondev, B.Pfeiffer, J.Blachot, X.Sun, M.MacCormick NUBASE2012 Evaluation of Nuclear Properties COMPILATION 197,212Bi; compiled experimental properties of nuclides, T1/2, J, π. Comparison with ENSDF library.
doi: 10.1016/j.nds.2014.06.127
2012AU07 Chin.Phys.C 36, 1157 (2012) G.Audi, F.G.Kondev, M.Wang, B.Pfeiffer, X.Sun, J.Blachot, M.MacCormick The NUBASE2012 evaluation of nuclear properties COMPILATION A=1-295; compiled, evaluated ground- and isomeric-states mass excess, J, π, decay properties.
doi: 10.1088/1674-1137/36/12/001
2012SU01 Phys.Rev. C 85, 014613 (2012) Pre-neutron-emission mass distributions for low-energy neutron-induced actinide fission NUCLEAR REACTIONS 235,238U, 237Np, 232Th, 239Pu(n, F), E=0.3-6 MeV; calculated pre-neutron-emission mass distributions, driving potential, phenomenological fission potential, energy dependence of the potential parameters, effect of nuclear deformations on potential parameters. Skyrme energy-density functional. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014613
2011HO01 Chin.Phys.C 35, 35 (2011) P.-Y.Hou, X.-J.Sun, C.-G.Yu, X.Lu Theoretical analysis of double-differential neutron emission cross sections for n+56Fe reactions at incident energies of 7-13 MeV NUCLEAR REACTIONS 56Fe(n, xn), E=7-13 MeV; calculated σ(θ, E). comparison with ENDF/B-VII.0 and JEFF-3.1 libraries, unified Hauser-Feshbach and exciton model.
doi: 10.1088/1674-1137/35/1/008
2011SU12 Chin.Phys.C 35, 555 (2011) X.-Y.Sun, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, J.-G.Chen, W.Guo, W.-D.Tian, H.-W.Wang, G.-Q.Zhang, P.Zhou A new probe of neutron skin thickness NUCLEAR REACTIONS 12C(50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), E = 50 MeV/nucleon; calculated neutron skin thickness vs. impact parameter. Isospin-Dependent Quantum Molecular Dynamics (IQMD) model.
doi: 10.1088/1674-1137/35/6/009
2010FU09 Nucl.Phys. A834, 584c (2010) Y.Fu, D.Q.Fang, Y.G.Ma, X.Z.Cai, X.Y.Sun, W.D.Tian Isoscaling in projectile fragmentation reaction induced by 40, 48Ca and 58, 64Ni NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated fragment yields using HIPSE (Heavy-Ion Phase Space Exploration) model; deduced isoscaling behaviour.
doi: 10.1016/j.nuclphysa.2010.01.098
2010SU07 Phys.Lett. B 682, 396 (2010) X.Y.Sun, D.Q.Fang, Y.G.Ma, X.Z.Cai, J.G.Chen, W.Guo, W.D.Tian, H.W.Wang Neutron/proton ratio of nucleon emissions as a probe of neutron skin NUCLEAR REACTIONS 12C(50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), E=50 MeV/nucleon; calculated neutron/proton yield ratio and dependence on neutron skin thickness using isospin-dependent quantum molecular model.
doi: 10.1016/j.physletb.2009.11.031
2010SU16 Int.J.Mod.Phys. E19, 1823 (2010) X.Y.Sun, J.G.Chen, D.Q.Fang, Y.G.Ma, X.Z.Cai, W.Guo, W.D.Tian, H.W.Wang, P.Zhou, G.Q.Zhang, X.G.Cao, Y.Fu, Z.G.Hu, J.S.Wang, M.Wang, Y.Togano, N.Aoi, H.Baba, T.Honda, K.Okada, Y.Hara, K.Ieki, Y.Ishibashi, Y.Itou, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Oishi, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, T.Motobayashi Measurement of the proton-proton correlation function from the break-up of 22Mg and 20Ne NUCLEAR REACTIONS 12C(22Mg, p), (20Ne, p), E=70 MeV/nucleon; measured reaction products, proton spectrum; deduced angular and momentum correlations between two protons, space-time information.
doi: 10.1142/S0218301310016259
2010SU19 Nucl.Phys. A834, 502c (2010) X.Y.Sun, D.Q.Fang, Y.G.Ma, X.Z.Cai, X.G.Cao, Y.Fu, W.D.Tian Dependence of n/p with neutron skin thickness for neutron-rich nuclei NUCLEAR REACTIONS 12C(50Ca, n), (50Ca, p), (52Ca, n), (52Ca, p), (54Ca, n), (54Ca, p), (56Ca, n), (56Ca, p), (60Ni, n), (60Ni, p), (62Ni, n), (62Ni, p), (64Ni, n), (64Ni, p), (66Ni, n), (66Ni, p), (68Ni, n), (68Ni, p), (70Ni, n), (70Ni, p), E=50 MeV/nucleon; calculated neutron-, proton-yields dependence on neutron skin, reduced impact and diffuseness parameters, rapidity using isospin-dependent quantum molecular dynamics model.
doi: 10.1016/j.nuclphysa.2010.01.077
2010ZH15 Int.J.Mod.Phys. E19, 957 (2010) P.Zhou, D.Q.Fang, Y.G.Ma, X.Z.Cai, J.G.Chen, W.Guo, X.Y.Sun, W.D.Tian, H.W.Wang, G.Q.Zhang, X.G.Cao, Y.Fu, Z.G.Hu, J.S.Wang, M.Wang, Y.Togano, N.Aoi, H.Baba, T.Honda, K.Okada, Y.Hara, K.Ieki, Y.Ishibashi, Y.Itou, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Oishi, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, T.Motobayashi Measurement of two-proton correlation from the break-up of 23Al RADIOACTIVITY 23Al, 22Mg(2p) [from 12C(23Al, X), (22Mg, X), (21Na, X), (20Ne, X), E=60-70 MeV/nucleon]; measured decay products; deduced trajectories, di-proton emission.
doi: 10.1142/S0218301310015400
2009DU17 Phys.Rev. C 80, 064612 (2009) Predicted levels of 9Be based on a theoretical analysis of neutron double-differential cross sections at En=14.1 and 18 MeV NUCLEAR REACTIONS 9Be(n, 2n), (n, X), E=14.1, 18 MeV; analyzed outgoing energy-angular spectra, σ, σ(θ) using statistical theory for neutron induced-light nucleus reactions.
doi: 10.1103/PhysRevC.80.064612
2009FA12 Chin.Phys.C 33, 197 (2009) D.-Q.Fang, Y.Fu, X.-Y.Sun, X.-Z.Cai, W.Guo, W.-D.Tian, H.-W.Wang, Y.-G.Ma Scaling property in one-nucleon removal reactions induced by exotic nuclei NUCLEAR REACTIONS 12C(19C, X), E=70 MeV/nucleon; calculated reaction fragment parallel momentum distributions; deduced scaling properties, halo nuclei identification.
doi: 10.1088/1674-1137/33/3/007
2009QU04 Chin.Phys.C 33, 31 (2009) Theoretical calculation of kerma coefficients for n+16O reaction below 30 MeV NUCLEAR REACTIONS 16O(n, X), E=5-30 MeV; calculated kerma coefficients; deduced a new kerma coefficients formula.
doi: 10.1088/1674-1137/33/1/007
2008SU21 Phys.Rev. C 78, 054610 (2008); Publishers Note Phys.Rev. C 80, 029901 (2009) New calculation method of neutron kerma coefficients for carbon and oxygen below 30 MeV NUCLEAR REACTIONS 12C, 16O(n, p), (n, α), (n, d), (n, t), (n, 3He), (n, 6Li), E<30 MeV; calculated kerma coefficients. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.054610
2006WA06 J.Phys.(London) G32, 309 (2006) High-energy Drell-Yan dimuon process in a Glauber model NUCLEAR REACTIONS 1H(p, X), E at 800 GeV/c; calculated Drell-Yan invariant σ. 2H, Be, C, Fe, W(p, X), E=800 GeV; calculated Drell-Yan σ ratios, QCD corrections. Glauber model.
doi: 10.1088/0954-3899/32/3/006
2003ZH41 Nucl.Sci.Eng. 143, 90 (2003) Z.Zhang, X.Sun, C.Cai, Q.Shen, Y.Han Calculations for Proton-Induced Reactions Below 250 MeV on 208Pb and 209Bi Targets NUCLEAR REACTIONS 208Pb, 209Bi(p, p), (p, X), E=10-400 MeV; analyzed elastic σ(θ), total σ; deduced optical model parameters. 209Bi(p, n), (p, 3n), (p, 4n), E<250 MeV; 208Pb(p, xn), (p, xnp), E < 250 MeV; 208Pb, 209Bi(p, nX), (p, pX), (p, dX), (p, tX), (p, αX), (p, 3HeX), E < 250 MeV; calculated σ. 208Pb(p, nX), E=11-45 MeV; 209Bi(p, nX), E=45-225 MeV; calculated neutron spectra. 208Pb(p, X)208Bi/207Bi/205Pb/204Pb/202Pb/204Tl/194Hg, E < 250 MeV; 209Bi(p, X)209Po/208Po/208Bi/207Bi/205Pb/204Pb/202Pb, E < 250 MeV; calculated production σ.
doi: 10.13182/NSE03-A2321
2000HU12 Chin.Phys.Lett. 17, 483 (2000) W.-X.Huang, Y.-X.Guo, X.-F.Sun, X.-G.Lei, X.-H.Zhou, Z.Liu, Y.-H.Zhang, S.-F.Zhu, X.Xu, X.-C.Feng, M.-Y.Liu, Y.-X.Luo, S.-X.Wen, X.-G.Wu, G.-J.Yuan, G.-S.Li, C.-X.Yang Experimental Study of High-Spin States in 119Xe NUCLEAR REACTIONS 106Cd(16O, n2p), E=67-80 MeV; measured Eγ, Iγ, γγ-coin. 119Xe deduced high-spin levels, J, π, configurations.
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