NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = Sun Xiangfu Found 90 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1998HU28 High Energy Phys. and Nucl.Phys. (China) 22, 385 (1998) W.Huang, R.Ma, S.Xu, X.Xu, Y.Xie, Z.Li, Y.Ge, Y.Wang, C.Wang, T.Zhang, X.Sun, G.Jin, Y.Luo β-delayed proton emission precursor 87Mo
1998LI06 Eur.Phys.J. A 1, 125 (1998) Z.Liu, X.Sun, X.Zhou, X.Lei, Y.Guo, Y.Zhang, X.Chen, H.Jin, Y.Luo, S.X.Wen, C.X.Yang, G.J.Yuan, G.S.Li, X.A.Liu, W.D.Luo, Y.S.Chen High Spin States and Evidence for Octupole Correlations in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=100-120 MeV; measured Eγ, Iγ(θ), γγ-coin, γγ(t). 117Xe deduced high-spin levels, J, π, B(λ), configurations, isomeric states T1/2. Cranked shell-model calculations.
doi: 10.1007/s100500050042
1997HA25 Phys.Rev. C55, 2838 (1997) Temperature and Density Dependence of the Nucleon Mean Free Path in the Relativistic Mean Field Model
doi: 10.1103/PhysRevC.55.2838
1997LI45 High Energy Phys. and Nucl.Phys. (China) 21, 881 (1997) Z.Liu, X.Sun, Y.Guo, X.Lei, X.Chen, X.Zhou, Y.Zhang, H.Jin, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang, X.Liu Lifetime measurement of the negative-parity isomers in 117Xe
1997ZH43 High Energy Phys. and Nucl.Phys. (China) 21, 187 (1997) Y.Zhang, Q.Zhao, X.Zhou, H.Xu, Y.Guo, X.Lei, J.Lu, S.Zhu, Q.Gou, H.Jin, Z.Liu, Y.Luo, X.Sun, Y.Zhu Band Structure in Doubly Odd 170Ta
1997ZH45 High Energy Phys. and Nucl.Phys. (China) 21, 393 (1997) Y.Zhang, Q.Zhao, X.Zhou, X.Sun, X.Lei, Y.Guo, Z.Liu, X.Chen, Y.Zhu High-Spin States in 162Lu and Signature Inversion of Yrast Bands in Doubly Odd Nuclei Around A = 160 Mass Region
1996ZH40 High Energy Phys. and Nucl.Phys. (China) 20, 769 (1996) X.Zhou, X.Sun, Y.Guo, X.Lei, Z.Liu, Y.Zhang, X.Chen, H.Jin, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang High-Spin States in 198Bi
1995LI08 Nucl.Phys. A583, 221c (1995) Z.Liu, X.Sun, X.Zhou, X.Lei, Y.Zhang, H.Jin, Q.Pan, Y.Guo, X.Chen, Y.Luo, S.Wen, G.Yuan, C.Yang, W.Luo, Y.S.Chen, Z.Xing, X.Q.Chen Search for Positive Parity Bands in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=115 MeV; measured γγ-coin. 117,119,121,123,125,127Cs level schemes included. 117Xe deduced levels, J, π, band structure, configuration. Model comparison.
doi: 10.1016/0375-9474(94)00662-7
1995LI22 Z.Phys. A351, 363 (1995) Z.Liu, X.Sun, X.Zhou, X.Lei, Y.Zhang, H.Jin, Q.Pan, Y.Guo, X.Chen, Y.Luo, S.Wen, G.J.Yuan, G.S.Li, C.X.Yang, W.D.Luo, Y.S.Chen Observation of High Spin States in 117Xe NUCLEAR REACTIONS 92Mo(28Si, n2p), E=100-120 MeV; measured γγ-coin, DCO ratios. 117Xe deduced high-spin levels, J, π, γ multipolarity, band structure.
doi: 10.1007/BF01291140
1995LI67 High Energy Phys. and Nucl.Phys. (China) 19, 106 (1995) Z.Liu, X.Sun, X.Zhou, X.Lei, H.Jin, Y.Guo, Q.Pan, Y.Zhang, X.Chen, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang Identification of Excited States in 117Xe
1995SU08 Phys.Rev. C51, 2803 (1995) X.Sun, Z.Liu, X.Zhou, X.Lei, H.Jin, Q.Pan, Y.Zhang, Y.Guo, Y.Luo, S.Wen, G.Yuan, G.Li, C.X.Yang, Z.Xing, X.Q.Chen Observation of a Possible πh11/2 Band in 117Cs NUCLEAR REACTIONS 92Mo(28Si, X), E=115 MeV; measured Eγ, Iγ(E), γγ-coin. 117Cs deduced high-spin levels, J, π. Particle-plus-traxial rotor calculations.
doi: 10.1103/PhysRevC.51.2803
1995YA23 High Energy Phys. and Nucl.Phys. (China) 19, 959 (1995) W.Yang, S.Yuan, X.Zhang, X.Yu, W.Mou, Z.Li, Z.Gan, H.Liu, J.Guo, J.Zhong, X.Sun The Synthesis and γ Decay of New Heavy Neutron-Rich Nuclide 175Er
1995ZH08 Chin.Phys.Lett. 12, 4 (1995) X.Zhou, X.Sun, X.Lei, H.Jin, Z.Liu, Y.Zhang, Q.Pan, Y.Guo, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang On Beam Study of 198Bi Decay NUCLEAR REACTIONS 187Re(16O, 5n), E=100 MeV; measured γγ(t). RADIOACTIVITY 198Bi(β+), (EC) [from 187Re(16O, 5n), E=100 MeV]; measured γγ(t). 198Pb deduced levels, T1/2, γ-multipolarity.
1995ZH36 Z.Phys. A353, 3 (1995) X.Zhou, Y.Guo, X.Sun, X.Lei, X.Chen, Z.Liu, Y.Zhang, H.Jin, Y.Luo, S.X.Wen, G.J.Yuan, G.S.Li, C.X.Yang Observation of Isomeric States in 197Bi NUCLEAR REACTIONS 187Re(16O, 6n), E=85-105 MeV; measured γγ(t), γ(θ). 197Bi deduced high-spin levels, isomers, T1/2.
doi: 10.1007/BF01297715
1995ZH59 High Energy Phys. and Nucl.Phys. (China) 19, 961 (1995) X.Zhou, X.Sun, Y.Guo, X.Lei, Z.Liu, X.Chen, Y.Zhang, H.Jin, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang Study of Excited States in Neutron-Deficient 197Bi
1994TA27 Nucl.Instrum.Methods Phys.Res. B90, 383 (1994) C.Tan, Y.Xia, X.Liu, J.Liu, J.Li, H.Yang, X.Sun Range Distribution of Fluorine in 19F+-Implanted LiNbO3 NUCLEAR REACTIONS, ICPND 19F(p, αγ), E ≈ 0.87-0.915 MeV; measured γ yield vs E for different implantation E(19F) in LiNbO3; deduced flourine range distribution.
doi: 10.1016/0168-583X(94)95576-X
1994ZH02 Phys.Rev. C49, R592 (1994) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, J.Wang, Z.Li, Z.Qin, G.Guo, Y.Luo, J.Zylicz, J.-Y.Zhang Observation of the New Neutron-Rich Nuclide 208Hg NUCLEAR REACTIONS Pb(12C, X), E=30 MeV/nucleon; measured Eγ, Iγ, following 208Tl-decay; deduced evidence for 208Hg, production σ. RADIOACTIVITY 208Hg(β-) [from Pb(12C, X), E=30 MeV/nucleon]; measured Eγ, Iγ, decay curve; deduced T1/2. 208Tl transition deduced T1/2.
doi: 10.1103/PhysRevC.49.R592
1994ZH47 High Energy Phys. and Nucl.Phys. (China), Supplement 1, 18, 28 (1994) X.Zhou, X.Sun, X.Lei, H.Jin, Z.Liu, Y.Zhang, Q.Pan, Y.Guo, X.Chen, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang Study of Low-lying Level Structure in 198Pb
1994ZH49 High Energy Phys. and Nucl.Phys. (China) 18, 296 (1994) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, J.Wang, Z.Li, Z.Qin, G.Guo Identification of 208Hg
1993SU31 Chin.J.Nucl.Phys. 15, No 3, 223 (1993) X.Sun, J.Yu, Y.Guo, X.Lei, Y.Luo, J.Wang, X.Zhou, X.Xu, S.Wen, P.Weng, S.Li, C.Yang Three-Quasiparticle Band of 125Cs NUCLEAR REACTIONS 109Ag(19F, 2np), E=75 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 125Cs deduced levels, J, π, band structure.
1993XU04 Chin.J.Nucl.Phys. 15, No 1, 18 (1993) X.Xu, J.Guo, Y.Guo, X.Ou, H.Liu, X.Lei, X.Sun, Y.Luo, J.Wang, J.Yu, T.Wang, Y.Wang, X.Zhou, L.Xu, S.Zhou Proton Emitters Produced in 28Si + 28Si Reaction NUCLEAR REACTIONS 28Si(28Si, X), E=104-127.2 MeV; measured fragment spectra; deduced evidence for 53mCo, 53Ni. RADIOACTIVITY 53mCo(p); 53Ni(β+p) [from 28Si(28Si, X), E=104-127.2 MeV]; measured proton spectra, T1/2.
1993ZH07 Nucl.Phys. A553, 489c (1993) L.Zhang, S.Yuan, G.Jin, T.Zhang, J.Zhao, Q.Pan, W.Yang, X.Zhang, Y.Yang, S.Xu, Z.Zhao, J.Zheng, X.Sun, W.Li, Y.Luo, B.Wei Synthesis and Identification of New Heavy Nuclides Far Off Stability NUCLEAR REACTIONS Pb(12C, X), E=30 MeV/nucleon; measured γ-spectra; deduced evidence for 208Hg, production <σ>. RADIOACTIVITY 208Hg(β-) [from Pb(12C, X), E=30 MeV/nucleon]; 185Hf(β-) [from 186W(n, 2p), E=14 MeV]; measured γ-spectra, decay rates; deduced T1/2. 185Ta deduced new transition.
doi: 10.1016/0375-9474(93)90645-E
1993ZH35 Chin.J.Nucl.Phys. 15, No 3, 227 (1993) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, J.Wang, Z.Li, Z.Qin, G.Guo Observation of New Neutron-Rich Isotope 208Hg NUCLEAR REACTIONS Pb(12C, X), E=30 MeV/nucleon; measured γ spectra, decay curves; deduced evidence for 208Hg, production σ. RADIOACTIVITY 208Hg(β-) [from Pb(12C, X), E=30 MeV/nucleon]; measured γ spectra, decay curves; deduced T1/2.
1992AL17 Z.Phys. A344, 1 (1992) D.Alber, A.Berger, H.H.Bertschat, H.Grawe, H.Haas, H.Kluge, A.Kuhnert, H.E.Mahnke, K.H.Maier, R.Schubart, B.Spellmeyer, X.Sun, L.Wood Nuclear Structure Study of the Neutron Deficient Cadmium Isotopes 100,101,102Cd NUCLEAR REACTIONS 46,47Ti, 50Cr(58Ni, X), E=230, 945 MeV; measured pγ-, ppγ-, nγ-, nnγ-, nγγ-coin, nγγ(t); deduced evidence for 100,101Cd. 70Ge(36Ar, 2n2p), (36Ar, 4n2p), E=135 MeV; measured γ(θ, H, t). 100,101,102Cd deduced isomers g, J, π, T1/2, B(λ), γ-multipolarity, quadrupole moment. Shell model comparison.
doi: 10.1007/BF01291011
1992KU13 Phys.Rev. C46, 484 (1992) A.Kuhnert, D.Alber, H.Grawe, H.Kluge, K.H.Maier, W.Reviol, X.Sun, E.M.Beck, A.P.Byrne, H.Hubel, J.C.Bacelar, M.A.Deleplanque, R.M.Diamond, F.S.Stephens Observation of High-Spin States in the N = 84 Nucleus 152Er and Comparison with Shell-Model Calculations NUCLEAR REACTIONS 116Sn(40Ar, 4n), E=180 MeV; measured γγ-coin, γγγ(t), γ(ce)(t), γγ(θ). 152Er deduced levels, J, π, γ-multipolarity, δ. Model comparison.
doi: 10.1103/PhysRevC.46.484
1992SU14 Chin.J.Nucl.Phys. 14, No 4, 295 (1992) X.Sun, J.Wang, Y.Guo, X.Lei, Y.Luo, J.Yu, X.Xu, S.Wen, P.Wen, S.Li, X.Yang Identification of the πg9/2 Band New Levels in 121Cs NUCLEAR REACTIONS 112Sn(12C, 2np), E=60 MeV; measured γγ-coin. 121Cs deduced levels, J, π, band structure.
1992SU16 High Energy Phys. and Nucl.Phys. (China) 16, 62 (1992) X.Sun, J.Yu, Y.Guo, X.Lei, Y.Luo, J.Wang, X.Xu, S.Wen, P.Weng, S.Li, C.Yang Measurement of 125Ba High Spin States
1992SU17 High Energy Phys. and Nucl.Phys. (China) 16, 552 (1992) X.Sun, J.Yu, Y.Guo, X.Lei, Y.Luo, J.Wang, X.Xu, S.Wen, P.Weng, S.Li, C.Yang Study on the Excited States of 124Cs by Heavy Ion Reaction
1992SU18 High Energy Phys. and Nucl.Phys. (China) 16, 938 (1992) X.Sun, J.Wang, Y.Guo, X.Lei, Y.Luo, J.Yu, X.Xu, S.Wen, P.Weng, S.Li, C.Yang Observation of New Levels in 121Cs
1992ZH44 High Energy Phys. and Nucl.Phys. (China) 16, 767 (1992) L.Zhang, G.Jin, J.Zhao, W.Yang, Y.Yang, Z.Zhao, J.Zheng, X.Sun, Z.Li, Z.Qin, J.Wang, G.Guo New Neutron-Rich Isotope 208Hg
1990AL07 Z.Phys. A335, 265 (1990) D.Alber, H.H.Bertschat, H.Grawe, H.Haas, B.Spellmeyer, X.Sun First In-Beam Observation of 97Ag - The Three-Proton-Hole Spectrum in 100Sn NUCLEAR REACTIONS 46Ti(58Ni, 2npα), (58Ni, n2pα), (58Ni, 2n3pα), E=230 MeV; 64Zn(36Ar, 2np), E=130 MeV; measured γ(particle), γγ(particle)-coin, γ(t). 97Ag deduced levels, J, π, T1/2. 97Pd deduced isomer J, π, T1/2. 95Rh deduced levels, J, π. Shell model comparison. NUCLEAR STRUCTURE 97Ag, 95Rh, 100Sn; calculated levels. Shell model.
1990HE08 Phys.Rev. C41, 1553 (1990) J.Heese, N.Martin, C.J.Gross, W.Fieber, K.P.Lieb, A.Kuhnert, K.H.Maier, X.Sun Conversion Electron and Yrast State Measurements in 73Br NUCLEAR REACTIONS 40Ca(36Ar, 3p), E=130 MeV; 58Ni(24Mg, p2α), E=110 MeV; measured Eγ, Iγ, I(ce), γγ-, (e-)γ-coin. 73Br deduced levels J, π, γ-multipolarity, ICC, rotational bands. 73Kr deduced ground state J, π.
doi: 10.1103/PhysRevC.41.1553
1989SU12 Z.Phys. A333, 281 (1989) X.Sun, U.Rosengard, H.Grawe, H.Haas, H.Kluge, A.Kuhnert, K.H.Maier Conversion Electron Measurement of Isomeric Primary Transitions in 196,198,199,200,201Pb NUCLEAR REACTIONS 182,184,186W(18O, xn), E=85 MeV; 192Os(13C, xn), E=70 MeV; measured (ce)(ce)-, γ(ce)-coin. 196,198,199,200,201Pb deduced isomer, J, π, T1/2, decay, B(λ).
1988FA12 High Energy Phys. and Nucl.Phys. (China) 12, 229 (1988) W.Fan, Z.Zhao, X.Sun, W.Mu, J.Ma, W.Yang, X.Xie, L.Zhao, J.Yu The decay study of 73Br
1988LI35 J.Nucl.Radiochem. 2, 9 (1988) W.Li, T.Sun, X.Sun, T.Zhang, M.Zheng, T.Dong, M.Fu Charge Distribution in the Fission of 238U by 14.7 MeV Neutron NUCLEAR REACTIONS 238U(n, F)82Br/132I/136Cs/140La/95Zr/97Zr/99Mo/131I/134I/135I/138Cs/142La, E=14.7 MeV; measured fission products using radiochemical methods; deduced independent and cumulative fission yields.
1987AL08 Z.Phys. A327, 127 (1987) D.Alber, H.Grawe, H.Haas, B.Spellmeyer, X.Sun In-Beam Study of Neutron Deficient 100Cd NUCLEAR REACTIONS 46Ti(58Ni, 2n2p), E=230 MeV; measured Eγ, Iγ, γnn-, nγγ-coin. 100Cd deduced levels, J, π, isomer T1/2. In-beam γ-spectroscopy.
1987JI04 Scientica Sinica 30, 1267 (1987) Jin Juguang, Wang Songyue, Sun Xiaozhong, Wang Xiulan Measurement of 235U Hyperfine Structure and Isotope Shift Spectra with Laser Optogal-Vanic Spectroscopy NUCLEAR MOMENTS 235,238U; measured optical isotope shifts. 235U; measured hfs; deduced hyperfine constants.
1987SC14 Z.Phys. A327, 251 (1987) K.Schiffer, A.Dewald, A.Gelberg, R.Reinhardt, K.O.Zell, Sun Xianfu, P.von Brentano Two-Quasiparticle Bands in 126Ba NUCLEAR STRUCTURE 126Ba; calculated levels, two quasiparticle Routhians, (g(k)-g(R)/Q0), branching ratios, δ. NUCLEAR REACTIONS 116Sn(13C, 3nγ), E=46-61 MeV; measured Eγ, Iγ, Iγ(t), γγ-coin, γ(θ). 126Ba deduced levels, J, π, yrast sequence, δ. Enriched target, Ge detector.
1986SC11 Z.Phys. A323, 487 (1986) K.Schiffer, A.Dewald, A.Gelberg, R.Reinhardt, K.O.Zell, Sun Xianfu, P.v.Brentano Excited States in 126Ba NUCLEAR REACTIONS 116Sn(13C, 3n), E=54 MeV; measured Eγ, Iγ, γ(θ), σ(Eγ). 126Ba deduced levels, J, π, band structure, Routhians.
1986SC24 Nucl.Phys. A458, 337 (1986) K.Schiffer, A.Dewald, A.Gelberg, R.Reinhardt, K.O.Zell, Sun Xiangfu, P.von Brentano Band Crossings in 128Ba NUCLEAR REACTIONS 118Sn(13C, 3n), E=46-56 MeV; measured Eγ, Iγ(E), Iγ(θ), γγ-coin. 128Ba deduced levels, J, π, ICC, T1/2. Cranking model calculations, IBA-1 calculations. Enriched target, Ge-detector, mini-orange, spectrometer, pulsed beam.
doi: 10.1016/0375-9474(86)90360-X
1985SU03 Nucl.Phys. A436, 506 (1985) X.Sun, D.Bazzacco, W.Gast, A.Gelberg, U.Kaup, K.Schiffer, A.Dewald, R.Reinhardt, K.O.Zell, P.Von Brentano Excited States in 130Ba NUCLEAR REACTIONS 120Sn(13C, 3n), E=45-58 MeV; measured Eγ, Iγ(E), Iγ(θ), γγ-coin, K-conversion coefficient. 130Ba deduced levels J, π, ICC. Cranking-model calculation. Enriched target. Ge(Li) detector, mini-orange spectrometer.
doi: 10.1016/0375-9474(85)90083-1
1983LI24 J.Nucl.Radiochem. 5, 176 (1983) W.Li, T.Sun, M.Zhen, T.Dong, X.Sun Determination of the Yields for the Rare-Earth Nuclides from 14 MeV Neutron Fission of 238U Using Ge(Li) Detector NUCLEAR REACTIONS 238U(n, F)93Y/141Ce/142La/143Ce/144Ce/145Pr/147Nd/149Nd/149Pm/151Pm/153Sm/156Sm/156Eu/157Eu, E=14 MeV; measured fission products, Eγ, Iγ; deduced cumulative yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32628. 1983SC37 Z.Phys. A313, 245 (1983) K.Schiffer, A.Dewald, A.Gelberg, R.Reinhardt, K.O.Zell, P.von Brentano, Sun Xiangfu Excited States in 128Ba NUCLEAR REACTIONS 118Sn(13C, 3n), E=46-56 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), σ(Eγ), I(ce). 128Ba deduced levels, γ-branching, J, π, γ-transition multipolarity.
doi: 10.1007/BF01417235
1983SU09 Phys.Rev. C28, 1167 (1983) Sun Xiangfu, D.Bazzacco, W.Gast, A.Gelberg, U.Kaup, A.Dewald, K.O.Zell, P.von Brentano Band Crossing in 130Ba NUCLEAR REACTIONS 120Sn(13C, 3nγ), E=45-58 MeV; measured Iγ, γγ-coin, σ(Eγ, θ), σ(Eγ, E). 130Ba deduced levels, J, π, γ-branching, backbending plots. Cranking model.
doi: 10.1103/PhysRevC.28.1167
Back to query form |