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NSR database version of April 11, 2024.

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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
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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
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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
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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
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2023SU02      Phys.Rev. C 107, L011601 (2023)

X.-X.Sun, L.Guo

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
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2023SU05      Phys.Rev. C 107, 064609 (2023)

X.-X.Sun, L.Guo

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2022SU07      Phys.Rev. C 105, 034601 (2022)

X.-X.Sun, L.Guo, A.S.Umar

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
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2022SU09      Phys.Rev. C 105, 044312 (2022)

X.Sun, J.Meng

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
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2022SU10      Phys.Rev. C 105, 054610 (2022)

X.-X.Sun, L.Guo

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
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2022SU20      Phys.Rev. C 106, 024334 (2022)

X.Sun, J.Meng

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
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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
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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
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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
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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
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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
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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
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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
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2021SU09      Phys.Rev. C 103, 044603 (2021)

X.Sun

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
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2021SU10      Phys.Rev. C 103, 054315 (2021)

X.-X.Sun

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
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2021SU23      Phys.Rev. C 104, 064319 (2021)

X.-X.Sun, S.-G.Zhou

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2689.


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


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32800.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0229.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0235.


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


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


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2616.


2020SU20      Nucl.Phys. A1003, 122011 (2020)

X.-X.Sun, J.Zhao, S.-G.Zhou

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32798.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32804.


2019SU11      Phys.Rev. C 99, 054604 (2019)

X.Sun, J.Chen, D.Lu

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32797.


2019SU26      Phys.Rev. C 100, 054605 (2019)

X.Sun, J.Chen, D.Lu

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32795.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2284. Data from this article have been entered in the XUNDL database. For more information, click here.


2018SU01      Chin.Phys.C 42, 014101 (2018)

X-W.Sun, J.Chen, D.-H.Lu

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
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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
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2018SU09      J.Phys.(London) G45, 075106 (2018)

X.-D.Sun, H.-F.Zhang

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
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2018SU18      Phys.Rev. C 98, 024607 (2018)

X.Sun, J.Chen, D.Lu

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
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2018SU22      Phys.Lett. B 785, 530 (2018)

X.-X.Sun, J.Zhao, S.-G.Zhou

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


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
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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
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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
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2017SU24      Phys.Rev. C 96, 024614 (2017)

X.Sun, D.Lu

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
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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
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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
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2016SU04      Phys.Rev. C 93, 014609 (2016)

X.Sun, J.Zhang

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
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2016SU09      Phys.Rev. C 93, 034316 (2016)

X.-D.Sun, P.Guo, X.-H.Li

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
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2016SU19      Phys.Rev. C 94, 024338 (2016)

X.-D.Sun, P.Guo, X.-H.Li

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
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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
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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
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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
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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
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2015SU13      Phys.Rev. C 92, 061601 (2015)

X.Sun, J.Zhang

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
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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
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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
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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
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2012SU01      Phys.Rev. C 85, 014613 (2012)

X.Sun, C.Yu, N.Wang

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
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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
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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
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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
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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
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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
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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
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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
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2009DU17      Phys.Rev. C 80, 064612 (2009)

J.Duan, J.Zhang, H.Wu, X.Sun

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
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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
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2009QU04      Chin.Phys.C 33, 31 (2009)

W.-J.Qu, J.-F.Liu, X.-J.Sun

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
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2008SU21      Phys.Rev. C 78, 054610 (2008); Publishers Note Phys.Rev. C 80, 029901 (2009)

X.Sun, W.Qu, J.Duan, J.Zhang

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
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2006WA06      J.Phys.(London) G32, 309 (2006)

H.-M.Wang, X.-J.Sun

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
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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
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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.


2000WA34      Chin.Phys.Lett. 17, 711 (2000)

N.Wang, X.-Z.Wu, Z.-X.Li, N.Wang, Y.-Z.Zhuo, X.-Q.Sun

Behavior of the Lyapunov Exponent and Phase Transition in Nuclei

NUCLEAR STRUCTURE 40,50Ca, 208Pb; calculated Lyapunov exponent vs temperature, phase transition features.


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Note: The following list of authors and aliases matches the search parameter X.Sun: , X.D.SUN, X.F.SUN, X.H.SUN, X.J.SUN, X.M.SUN, X.Q.SUN, X.X.SUN, X.Y.SUN