NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.Cai Found 61 matches. 2024AP01 Eur.Phys.J. C 84, 138 (2024) E.Aprile, K.Abe, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, M.Bazyk, L.Bellagamba, R.Biondi, A.Bismark, E.J.Brookes, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, J.M.R.Cardoso, D.Cichon, A.P.Cimental Chavez, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, J.P.Cussonneau, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, M.Flierman, W.Fulgione, C.Fuselli, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Glade-Beucke, L.Grandi, J.Grigat, H.Guan, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, N.F.Hood, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, A.Molinario, S.Moriyama, K.Mora, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, Q.Pellegrini, R.Peres, C.Peters, J.Pienaar, M.Pierre, G.Plante, T.R.Pollmann, J.Qi, J.Qin, D.Ramirez Garcia, N.Sarcevic, J.Shi, R.Singh, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, V.H.S.Wu, Y.Xing, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu, XENON collaboration Design and performance of the field cage for the XENONnT experiment
doi: 10.1140/epjc/s10052-023-12296-y
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
2023AP04 Phys.Rev. D 108, 072015 (2023) E.Aprile, K.Abe, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, M.Bazyk, L.Bellagamba, R.Biondi, A.Bismark, E.J.Brookes, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, J.M.R.Cardoso, A.P.Cimental Chavez, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, M.Flierman, W.Fulgione, C.Fuselli, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Glade-Beucke, L.Grandi, J.Grigat, H.Guan, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, N.F.Hood, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, D.G.Layos Carlos, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, A.Molinario, S.Moriyama, K.Moraa, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, Q.Pellegrini, R.Peres, C.Peters, J.Pienaar, M.Pierre, G.Plante, T.R.Pollmann, J.Qi, J.Qin, D.Ramirez Garcia, J.Shi, R.Singh, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, V.H.S.Wu, Y.Xing, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu Search for events in XENON1T associated with gravitational waves
doi: 10.1103/PhysRevD.108.072015
2022AP04 Phys.Rev.Lett. 129, 161805 (2022) E.Aprile, K.Abe, F.Agostini, S.Ahmed Maouloud, L.Althueser, B.Andrieu, E.Angelino, J.R.Angevaare, V.C.Antochi, D.Anton Martin, F.Arneodo, L.Baudis, A.L.Baxter, L.Bellagamba, R.Biondi, A.Bismark, A.Brown, S.Bruenner, G.Bruno, R.Budnik, T.K.Bui, C.Cai, C.Capelli, J.M.R.Cardoso, D.Cichon, M.Clark, A.P.Colijn, J.Conrad, J.J.Cuenca-Garcia, J.P.Cussonneau, V.D'Andrea, M.P.Decowski, P.Di Gangi, S.Di Pede, A.Di Giovanni, R.Di Stefano, S.Diglio, K.Eitel, A.Elykov, S.Farrell, A.D.Ferella, C.Ferrari, H.Fischer, W.Fulgione, P.Gaemers, R.Gaior, A.Gallo Rosso, M.Galloway, F.Gao, R.Gardner, R.Glade-Beucke, L.Grandi, J.Grigat, M.Guida, R.Hammann, A.Higuera, C.Hils, L.Hoetzsch, J.Howlett, M.Iacovacci, Y.Itow, J.Jakob, F.Joerg, A.Joy, N.Kato, M.Kara, P.Kavrigin, S.Kazama, M.Kobayashi, G.Koltman, A.Kopec, F.Kuger, H.Landsman, R.F.Lang, L.Levinson, I.Li, S.Li, S.Liang, S.Lindemann, M.Lindner, K.Liu, J.Loizeau, F.Lombardi, J.Long, J.A.M.Lopes, Y.Ma, C.Macolino, J.Mahlstedt, A.Mancuso, L.Manenti, F.Marignetti, T.Marrodan Undagoitia, K.Martens, J.Masbou, D.Masson, E.Masson, S.Mastroianni, M.Messina, K.Miuchi, K.Mizukoshi, A.Molinario, S.Moriyama, K.Mora, Y.Mosbacher, M.Murra, J.Muller, K.Ni, U.Oberlack, B.Paetsch, J.Palacio, P.Paschos, R.Peres, C.Peters, J.Pienaar, M.Pierre, V.Pizzella, G.Plante, J.Qi, J.Qin, D.Ramirez Garcia, S.Reichard, A.Rocchetti, N.Rupp, L.Sanchez, J.M.F.dos Santos, I.Sarnoff, G.Sartorelli, J.Schreiner, D.Schulte, P.Schulte, H.Schulze Eissing, M.Schumann, L.Scotto Lavina, M.Selvi, F.Semeria, P.Shagin, S.Shi, E.Shockley, M.Silva, H.Simgen, J.Stephen, A.Takeda, P.-L.Tan, A.Terliuk, D.Thers, F.Toschi, G.Trinchero, C.Tunnell, F.Tonnies, K.Valerius, G.Volta, Y.Wei, C.Weinheimer, M.Weiss, D.Wenz, C.Wittweg, T.Wolf, D.Xu, Z.Xu, M.Yamashita, L.Yang, J.Ye, L.Yuan, G.Zavattini, M.Zhong, T.Zhu Search for New Physics in Electronic Recoil Data from XENONnT RADIOACTIVITY 124Xe(2EC); measured decay products, X-rays; deduced T1/2. Comparison with available data. The XENONnT experiment, located at the INFN Laboratori Nazionali del Gran Sasso (LNGS) in Italy, was designed as a fast upgrade of XENON1T and inherits many of its systems such as cooling, gas storage, purification, and Kr removal.
doi: 10.1103/PhysRevLett.129.161805
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
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
2021GU15 Ann.Nucl.Energy 158, 108248 (2021) H.Guo, W.Chen, T.Ye, W.Sun, Y.Han, C.Cai Theoretical calculation of n+235U reaction NUCLEAR REACTIONS 235U(n, X)1NN/1H/2H/3H/3He/4He, E<150 MeV; calculated particle emission and γ-ray production σ, σ(θ), σ(θ, E). Comparison with ENDF/B-VIII.0 and JENDL-4.0 evaluated libraries.
doi: 10.1016/j.anucene.2021.108248
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
2020GU07 Ann.Nucl.Energy 142, 107363 (2020) H.Guo, W.Chen, T.Ye, W.Sun, Y.Han, C.Cai Theoretical calculation and evaluation of N + 237, 241, 243, 245Pu reactions NUCLEAR REACTIONS 237Pu(n, F), 241Pu(n, X), (n, γ), (n, F), Pu(n, X), (n, n'), (n, 2n), E<20 MeV; calculated σ using the optical model, distorted wave Born approximation theory, Hauser-Feshbach theory with width fluctuation correction, fission model, evaporation model, exciton model and the intranuclear cascade model. Comparison with ENDF/B-VIII, JENDL-4.0/HE and TENDL libraries.
doi: 10.1016/j.anucene.2020.107363
2020XU03 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 12C, 27Al, 28Si, 58Ni, 208Pb(8B, 8B), 9Be, 12C, 16O, 28Si, 58Ni, 120Sn, 208Pb(10B, 10B), 12C, 28Si, 58Ni, 208Pb, 209Bi(11B, 11B), E<50 MeV; analyzed available data. 8,10,11B; calculated σ; deduced global phenomenological optical model potentials.
doi: 10.1088/1674-1137/44/3/034101
2020XU04 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 27Al, 58Ni, 208Pb, 12C, 28Si(8B, 8B), E<100 MeV; 27Al, 28Si, 58Ni, 120Sn, 16O, 9Be, 208Pb(10B, 10B), E<100 MeV; 28Si, 58Ni, 209Bi, 12C, 209Bi(11B, 11B), E<100 MeV; analyzed available data. 9Be; deduced optical model potential parameters, σ, σ(θ).
doi: 10.1088/1674-1137/44/3/034101
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
2019XU05 Phys.Rev. C 99, 034618 (2019) Y.Xu, Y.Han, H.Liang, Z.Wu, H.Guo, C.Cai Global optical model potential for the weakly bound projectile 9Be NUCLEAR REACTIONS Mg(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 27Al(9Be, 9Be), E=12.0, 14.0, 18.0, 20.0, 22.0, 25.0, 28.0, 32.0, 33.0, 35.0.40.0, 47.5 MeV; 28Si(9Be, 9Be), E=12.0, 13.0, 14.0, 17.0, 20.0, 23.0, 26.0, 30.0, 45.0, 50.0, 60.0 MeV; 40Ca(9Be, 9Be), E=14.0, 20.0, 26.0, 45.0.50.0, 60.0 MeV; 58Ni(9Be, 9Be), E=20.0, 26.0 MeV; 64Zn(9Be, 9Be), E=17.0, 19.0, 21.0, 23.0, 26.0, 28.0, 28.4, 28.97 MeV; 89Y(9Be, 9Be), E=18.6, 20.6, 22.7, 24.7, 26.7, 28.7, 33.2 MeV; Ag(9Be, 9Be), E=26.0 MeV; 144Sm(9Be, 9Be), E=30.0, 31.5, 33.0, 34.0, 35.0, 37.0, 39.0, 41.0, 44.0, 48.0 MeV; 208Pb(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 9.5, 40.0, 41.0, 42.0, 44.0, 46.0, 47.2, 48.0, 50.0, 60.0, 68.0, 75.0 MeV; 209Bi(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 39.5, 40.0, 41.0, 42.0, 44.0, 46.0, 48.0 MeV; analyzed elastic σ(θ, E) data for global phenomenological energy-dependent optical model potential parameters for 9Be. 9Be, 12,13C, 27Al, 64Zn, 89Y, 144Sm(9Be, X), E=10-300 MeV; 28Si, Cu(9Be, X), E=10-500 MeV; 89Y(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (9Be, X), (11B, X); calculated reaction σ(E) using optical model and compared with experimental data. 9Be(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 12C(9Be, 9Be), E=13.0, 14.0, 14.5, 17.3, 19.0, 20.0, 21.0, 26.0, 153.8 MeV; 13C(9Be, 9Be), E=19.46, 25.05 MeV; 16O(9Be, 9Be), E=20.0, 25.94 MeV; calculated elastic σ(θ, E) using optical model parameters and compared with experimental data.
doi: 10.1103/PhysRevC.99.034618
2018GU18 Chin.Phys.C 42, 124101 (2018) Double differential cross sections of light charged particle production for the n+238U reaction NUCLEAR REACTIONS 238U(n, X)1H/2H/3H/4He, E<150 MeV; calculated fission σ, ←E). Comparison with ENDF/B-VII, JENDL-4. evaluated libraries.
doi: 10.1088/1674-1137/42/12/124101
2018XU01 Phys.Rev. C 97, 014615 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai Global phenomenological optical model potential for the 7Li projectile nucleus NUCLEAR REACTIONS 9Be(7Li, 7Li), E=15.75, 24.0, 30.0, 63.0, 130.0 MeV; 12C(7Li, 7Li), E=7.5, 9.0, 12.0, 15.0, 36.0, 131.8 MeV; 16O(7Li, 7Li), E=26.0, 36.0, 42.0, 50.0 MeV; 11B, 12,13C, 24Mg(7Li, 7Li), E=34.0 MeV; 24,26Mg(7Li, 7Li), E=88.7 MeV; 27Al(7Li, 7Li), E=6.0, 7.0, 8.0, 9.0, 10.0, 11.0, 12.0, 13.0, 14.0, 16.0, 18.0, 19.0, 24.0 MeV; 28Si(7Li, 7Li), E=8.0, 8.5, 9.0, 10.0, 11.0, 11.5, 13.0, 15.0, 16.0, 21.0, 26.0, 36.0, 177.8 MeV; 40,44,48Ca(7Li, 7Li), E=34.0; 40Ca(7Li, 7Li), E=88.7 MeV; 46,48Ti(7Li, 7Li), E=17.0 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe, 65Cu, 90Zr(7Li, 7Li), E=34.0 MeV; 58Ni(7Li, 7Li), E=14.22, 16.25.18.28, 19.0, 20.31.34.0, 42.0 MeV; 60,62Ni, 64,68Zn(7Li, 7Li), E=34.0 MeV; 80Se(7Li, 7Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 23.0, 26.0 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 116Sn(7Li, 7Li), E=18.0, 19.0, 20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0 MeV; 120Sn(7Li, 7Li), E=19.5, 20.0, 20.5, 22.0, 24.0, 25.0, 26.0, 28.0, 30.044.0 MeV; 138Ba(7Li, 7Li), E=21.0, 22.0, 23.0, 24.0, 28.0, 30.0, 32.0, 52.0 MeV; 140Ce, 142Nd(7Li, 7Li), E=52.0 MeV; 144Sm(7Li, 7Li), E=21.6, 22.1, 22.6.23.0, 25.0, 27.0, 29.0, 30.0, 32.0, 35.0, 40.8, 52.0 MeV; 208Pb(7Li, 7Li), E=27.0, 29.0, 33.0, 39.0, 42.0, 52.0 MeV; 232Th(7Li, 7Li), E=24.0, 26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed σ(θ, E) experimental data by global phenomenological optical model potential. 13C, 27Al, 64Zn, 116Sn, 138Ba, (7Li, X), E<300 MeV; 28Si, Cu, 208Pb(7Li, X), E<400 MeV; calculated reaction σ(E) using optical model, and compared with experimental data.
doi: 10.1103/PhysRevC.97.014615
2018XU10 Phys.Rev. C 98, 024619 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai 6Li global phenomenological optical model potential NUCLEAR REACTIONS 24Mg, 48Ca(6Li, 6Li), E=240.0 MeV; 25,26Mg, 39K, 91Zr(6Li, 6Li), E=34.0 MeV; 27Al(6Li, 6Li), E=7.0, 8.0, 10.0, 12.0, 18.0, 34.0 MeV; 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 16.0, 20.0, 21.0, 25.0, 27.0, 34.0, 46.0, 99.0, 135.0, 154.0, 210.0, 240.0, 318.0, 350.0 MeV; 40Ca(6Li, 6Li), E=50.6, 99.0, 156.0, 210.0, 240.0 MeV; 54Fe(6Li, 6Li), E=38.0, 44.0, 50.0 MeV; 59Co(6Li, 6Li), E=12.0, 18.0, 26.0, 30.0 MeV; 58Ni(6Li, 6Li), E=9.85, 11.21, 12.13, 13.04, 14.04, 34.0, 50.6, 73.7, 90.0, 99.0, 210.0, 240.0 MeV; 65Cu(6Li, 6Li), E=25.0 MeV; 64Zn(6Li, 6Li), E=10.77, 11.69, 12.0, 12.43, 13.0, 13.54, 13.8, 14.92, 15.0, 16.30, 16.5, 18.0, 18.14, 19.98, 22.0 MeV; 72,74,76Ge(6Li, 6Li), E=28.0 MeV; 80Se(6Li, 6Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 22.19, 23.0, 26.0 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=11.0, 12.0, 13.0, 15.0, 17.0, 19.0, 21.0, 25.0, 30.0, 34.0, 60.0, 70.0, 73.7, 99.0, 156.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 112Sn(6Li, 6Li), E=21.0, 22.0, 23.0, 25.0, 30.0, 35.0 MeV; 116Sn(6Li, 6Li), E=20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0, 40.0 MeV; 118Sn(6Li, 6Li), E=42.0 MeV; 120Sn(6Li, 6Li), E=30.0, 44.0, 90.0 MeV; 124Sn(6Li, 6Li), E=73.7 MeV; 138Ba(6Li, 6Li), E=21.0, 22.0, 23.0, 24.0, 26.0, 28.0 MeV; 144Sm(6Li, 6Li), E=21.0, 22.1, 22.6, 24.1, 26.0, 28.0, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25.0, 29.0, 31.0, 33.0, 35.0, 36.0, 37.0, 39.0, 42.0, 43.0, 46.0, 48.0, 50.6, 73.7, 88.0, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=24.0, 26.0, 28.0, 29.9, 30.0, 32.0, 32.8, 34.0, 36.0, 40.0, 44.0, 50.0 MeV; 232Th(6Li, 6Li), E=26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed differential σ(θ, E) data; deduced a new set of 6Li global phenomenological energy-dependent optical potential parameters based on the form of the Woods-Saxon potential within the optical model. 63,65Cu, 64Zn, 112,116Sn, 138Ba, 208Pb(6Li, X), E<400 MeV; calculated reaction σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.98.024619
2017GU06 Phys.Rev. C 95, 034614 (2017) H.Guo, H.Liang, Y.Xu, Y.Han, Q.Shen, C.Cai, T.Ye Microscopic optical potential for 6He NUCLEAR REACTIONS 12C(6He, 6He), E=8.79, 9.18, 9.9, 18, 230, 250 MeV; 27Al(6He, 6He), E=9.54, 11.0, 12.0, 13.4 MeV; 51V(6He, 6He), E=15.4, 23.0 MeV; 58Ni(6He, 6He), E=9.0, 10.0, 12.2, 16.5, 21.7 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 65Cu(6He, 6He), E=19.56, 22.6, 30.05 MeV; 120Sn(6He, 6He), E=17.4, 18.05, 19.8, 20.05 MeV; 197Au(6He, 6He), E=10.1, 27.0 MeV; 209Bi(6He, 6He), E=14.71, 16.26, 17.8, 19.0, 19.14, 22.02, 22.5 MeV; 208Pb(6He, 6He), E=14.0, 16, 18, 22, 27, 56.6 MeV; 9Be(6He, 6He), E=16.2, 16.8, 21.3, 150 MeV; calculated differential σ(θ, E) relative to Rutherford cross section using microscopic optical potential (MOP) and global phenomenological 6He optical potential (GOP) based on experimental data. 28Si(6He, X), E<330 MeV; calculated total σ(E) using MOP and GOP. Comparison with experimental data. Isospin-dependent nucleon microscopic optical potential derived by using Green's function method through the nuclear matter approximation and the local density approximation based on the Skyrme nucleon-nucleon effective interaction.
doi: 10.1103/PhysRevC.95.034614
2017GU15 Ann.Nucl.Energy 108, 151 (2017) H.Guo, Y.Han, T.Ye, W.Sun, C.Cai Theoretical analysis and evaluation for neutron-induced reaction on 239Pu NUCLEAR REACTIONS 239Pu(n, X), (n, n), (n, n'), E<200 MeV; calculated σ, σ(θ, E). Comparison with ENDF/B-VII, JENDL-4 libraries, experimental data.
doi: 10.1016/j.anucene.2017.04.043
2017SU16 Phys.Rev. C 95, 054606 (2017) X.W.Su, Y.L.Han, H.Y.Liang, Z.D.Wu, H.R.Guo, C.H.Cai Global phenomenological optical model potential for 8Li projectile NUCLEAR REACTIONS 9Be(8Li, 8Li), E=14, 19.6, 27 MeV; 12C(8Li, 8Li), E=14, 23.9 MeV; 13C, 14N, 27Al, 197Au(8Li, 8Li), E=14 MeV; 51V(8Li, 8Li), E=18.5, 26 MeV; 58Ni(8Li, 8Li), E=14, 19.6, 20.2, 22 MeV; 208Pb(8Li, 8Li), E=24.4, 27.9, 28.9, 30.6, 33.1 MeV; calculated σ(θ, E) by optical potential model, and compared with experimental data; deduced global phenomenological optical model parameters (OMPs) for 8Li. 9Be(8Li, X), E=19.6 MeV; 12C(8Li, X), E=14 MeV; 51V(8Li, X), E=18.5, 26.0 MeV; 208Pb(8Li, X), E=24.4, 27.6, 28.89, 30.57, 33.13 MeV; calculated total σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.95.054606
2016SU02 Ann.Nucl.Energy 90, 123 (2016) Neutron-induced reaction on 233U NUCLEAR REACTIONS 233U(n, X), (n, n), (n, n'), (n, γ), (n, F), E<200 MeV; calculated σ, σ(E), σ(θ, E). Comparison with experimental data, ENDF/B-VII and JENDL-4 evaluated nuclear libraries.
doi: 10.1016/j.anucene.2015.12.003
2016SU13 Int.J.Mod.Phys. E25, 1650033 (2016) X.-W.Su, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Global 6He optical model potential NUCLEAR REACTIONS 6,7Li, 9Be, 12C, 27Al, 28Si, 51V, 48Ti, 58Ni, 63,65Cu, 64Zn, 120Sn, 197Au, 206,208Pb, 209Bi(6He, X), (6He, 6He), E<300 MeV; analyzed available data; deduced optical potential; calculated σ, σ(θ).
doi: 10.1142/S0218301316500336
2014HA16 Nucl.Data Sheets 118, 108 (2014) Y.Han, C.Cai, H.Guo, Z.Zhang, Q.Shen Present Status of Evaluated Nuclear Data Library for ADS in China COMPILATION 27Al(n, x), E=0.01-350 MeV; calculated σ. 27Al(n, xn), E=14.1 MeV; calculated σ(En, θ). 27Al(n, xp), (n, xn), E=≈30-62.7 MeV; calculated σ(Eout). 27Al(n, 3He), E=95.6 MeV; calculated σ(Eout, θ). 209Bi(p, 3n), (p, 2np), E=20-200 MeV; calculated σ. 209Bi(p, x), E=61.7 MeV; calculated σ(Eout, θ). UNF code (optical model plus unified HF plus exciton model); compared with data.
doi: 10.1016/j.nds.2014.04.012
2014HA17 Nucl.Data Sheets 118, 132 (2014) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculation of Actinide Nuclear Reaction Data
doi: 10.1016/j.nds.2014.04.018
2014SU19 Ann.Nucl.Energy 76, 469 (2014) Theoretical calculations of n+232Th reaction for energies up to 150 MeV NUCLEAR REACTIONS 232Th(n, γ), (n, F), (n, 2n), (n, xn), E<150 MeV; calculated σ, σ(θ, E), σ(E). Comparison with ENDF/B-VII, JENDL-3.3 libraries, experimental data.
doi: 10.1016/j.anucene.2014.10.021
2013HA04 Ann.Nucl.Energy 55, 75 (2013) Double differential cross sections of light charged particle emission of n + 27Al reaction NUCLEAR REACTIONS 27Al(n, xp), (n, xd), (n, xt), (n, xα), (n, 3He), E<40 MeV; calculated σ(E, θ), σ(E). Comparison with available data.
doi: 10.1016/j.anucene.2012.11.031
2012HA16 Ann.Nucl.Energy 46, 179 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen The analysis of n+237Np reactions for energies up to 200 MeV NUCLEAR REACTIONS 237Np(n, γ), (n, F), (n, 2n), (n, xn), (n, xp), (n, xd), (n, xt), (n, xα) E<200 MeV; calculated σ, σ(θ, E), σ(θ), σ(E). Optical model, the intra-nuclear cascade model, the unified Hauser-Feshbach theory, comparison with ENDF/B-VII and JENDL-3 libraries and available data.
doi: 10.1016/j.anucene.2012.03.013
2012HA24 Nucl.Sci.Eng. 172, 102 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculations and Analysis of n + 27Al Reaction NUCLEAR REACTIONS 27Al(n, X), (n, n), (n, n'), (n, p), (n, γ), (n, d), (n, t), (n, α), (n, 2n), (n, xn), (n, xp), (n, xα), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Comparison with ENDF/B-VII and JENDL-3 evaluated nuclear libraries.
doi: 10.13182/NSE11-28
2011HA44 J.Korean Phys.Soc. 59, 855s (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen, C.Cai The Theoretical Calculation of Cross Section and Spectrum for n+238U Reaction up to 150 MeV NUCLEAR REACTIONS 238U(n, f), (n, xn), (n, d), (n, t), (n, p), (n, α), E=0-200 MeV; calculated σ, dσ(E, θ) using different reaction models.
doi: 10.3938/jkps.59.855
2011HA46 J.Korean Phys.Soc. 59, 1069s (2011) Present Status of Evaluated Nuclear Data Library for Accelerator-Driven Systems in China COMPILATION 24,25,26Mg, 27Al, 28,29,30Si, 40,42,43,44,46,48Ca, 50,52,53,54Cr, 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 90,91,92,94,96Zr, 93Nb, 91,94,95,96,97,98,100Mo, 180,182,183,184,186W, 204,206,207,208Pb, 209Bi, 232Th, 237Np, 232,233,234,235,236,237,238,239,240U, 236,244,245,245Pu, 241,242m,242,243Am, 243,244,245,246,247,248Cm(n, X), (p, X), E=0-200 MeV; calculated, evaluated σ, σ(E, θ).
doi: 10.3938/jkps.59.1069
2010CA03 Nucl.Sci.Eng. 164, 304 (2010) Recalculation and Reevaluation of the Complete Sets of Neutron Data for 63Cu and 65Cu Below 20 MeV COMPILATION 63,65Cu; compiled evaluated nuclear reaction data.
doi: 10.13182/NSE08-62TN
2010HA01 Nucl.Sci.Eng. 164, 185 (2010) Double-Differential Cross Sections of the Particle Emission in Neutron-Induced Reactions on 209Bi NUCLEAR REACTIONS 209Bi(n, X), (n, n), (n, n'), (n, 2n), (n, 3n), (n, xp), (n, xn), (n, xd), (n, xt), (n, xt), (n, xα), E<200 MeV; calculated σ, σ(E), σ(θ), σ(θ, E). Comparison with experimental data.
doi: 10.13182/NSE09-20
2010SU15 Nucl.Instrum.Methods Phys.Res. B268, 2585 (2010) X.Su, H.Liang, Y.Han, C.Cai, Q.Shen The theoretical calculation of p+232Th reaction for energies up to 250 MeV NUCLEAR REACTIONS 232Th(p, n), (p, 2n), (p, 3n), (p, 6n), (p, xn), (p, xα), (p, xt), (p, F), (p, X), E<250 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Optical and Iwamoto-Harada models.
doi: 10.1016/j.nimb.2010.07.003
2010ZH02 Ann.Nucl.Energy 37, 130 (2010) Double differential cross sections of light charged particle emission in neutron induced reactions on 54, 56, 57, 58Fe NUCLEAR REACTIONS 54,56,57,58Fe(n, px), (n, dx), (n, tx), (n, αx), E<100 MeV; calculated energy spectra, σ(θ, E). Comparison with experimental data.
doi: 10.1016/j.anucene.2009.11.013
2009LI01 J.Phys.(London) G36, 015102 (2009) C.-T.Liang, Y.-A.Luo, X.-H.Li, C.-H.Cai Systematic analysis of the reaction cross section for d, 3He and 4He as projectiles NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40,48Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(d, X), (3He, X), (α, X), E < 100 MeV/nucleon; calculated total reaction cross sections.
doi: 10.1088/0954-3899/36/1/015102
2009LI09 Eur.Phys.J. A 39, 255 (2009) The folding deuteron optical model potentials NUCLEAR REACTIONS 6Li, 9Be, 11B, 12,13C, 14N, 16O, 20,22Ne, 24Mg, 27Al, 28Si, 32S, 40Ar, 39K, 40,44,48Ca, 48,49,50Ti, 51V, 52Cr, 54,56,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 68Zn, 74Ge, 86Sr, 89Y, 90,91,92,94,96Zr, 93Nb, 92,100Mo, 103Rh, 105Pd, 112Cd, 115In, 112,116,118,120,124Sn, 140Ce, 165Ho, 181Ta, 197Au, 206,208Pb, 209Bi, 232Th, 238U(d, X), E<97.4 MeV; calculated elastic and non-elastic σ(θ, E). Comparison of new optical model potential with ten others and experimental data.
doi: 10.1140/epja/i2008-10718-y
2009LI26 J.Phys.(London) G36, 085104 (2009) Global 3He optical model potential below 270 MeV NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 14N, 16,17,18O, 20,22Ne, 23Na, 24,25,26Mg, 27Al, 28Si, 31P, 40Ar, 40,44,48Ca, 51V, 52Cr, 54,56Fe, 59Co, 58,60,61,62,64Ni, 89Y, 90,92,94Zr, 105Pd, 114Cd, 115In, 116,118,120Sn, 144,148,150,152,154Sm, 197Au, 205Tl, 208Pb(N, N), E ≤ 270 MeV; calculated σ, σ(θ); deduced 3He optical model potential parameters. Code CAPMN, comparison with experiment.
doi: 10.1088/0954-3899/36/8/085104
2009LI60 Chin.Phys.C 33, 415 (2009) Comparison between global phenomenological and microscopic optical potentials for proton as projectile below 100 MeV NUCLEAR REACTIONS Mg, Al, Si, P, S, Cl, Ar, K, Ca, Sc, Ti, V, Cr, Fe, Co, Ni, Cu, Zn, Ge, Se, Sr, Y, Zr, Mo, Rh, Pd, Cd, In, Sn, Te, Ba, La, Ce, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb, Hf, Ta, W, Os, Pt, Au, Pb, Bi, Th, U(p, p), E<100MeV; calculated incoming proton σ, elastic scattering σ(θ). Optical model potentials.
doi: 10.1088/1674-1137/33/6/003
2008HA33 Ann.Nucl.Energy 35, 2031 (2008) Double differential cross sections of neutron and proton emission in neutron induced reactions on 54, 56, 57, 58Fe NUCLEAR REACTIONS 56Fe(n, X), (n, pX), (n, nX), E < 200 MeV; 54,57,58Fe(n, pX), E < 200 MeV; calculated σ(θ, E). Compared results to available data.
doi: 10.1016/j.anucene.2008.06.002
2008LI05 Nucl.Phys. A801, 43 (2008) Global dispersive optical model potential for proton as projectile in the energy region up to 200 MeV NUCLEAR REACTIONS 24,26Mg, 27Al, 28Si, 31P, 40Ar, 40,42,44,48Ca, 45Sc, 46,48,50Ti, 51V, 50,52Cr, 55Mn, 54,56,57,58Fe, 59Co, 58,60,62,64Ni, 63,65Cu, 64,66,68,70Zn, 70Ge, 74,76,78,80,82Se, 86,88Sr, 89Y, 90,91,92,94,96Zr, 92,94,96,98,100Mo, 102Ru, 104,106,108,110Pd, 106,108,110,111,112,113,114,116Cd, 116,120,124Sn, 134,136,138Ba, 144Nd, 144,148,150,152,154Sm, 160Gd, 164Dy, 165Ho, 166,168Er, 172,174,176Yb, 178,180Hf, 182,184,186W, 188,190,192Os, 194,198Pt, 197Au, 206,207,208Pb, 209Bi, 232Th, 235,238U(p, p), E≈1-200 MeV; calculated σ(θ). 112,114,116,118,120,122,124Sn(p, p'), E=0-200 MeV; calculated nonelastic σ. New global proton dispersive optical model parameters. Comparison with Koning and Delaroche potential.
doi: 10.1016/j.nuclphysa.2007.12.004
2007LI41 Nucl.Sci.Eng. 157, 159 (2007) Calculation and Analysis for p + 58, 60, 61, 62, 64Ni Reactions Below 200 MeV NUCLEAR REACTIONS 58,60,61,62,64Ni(p, X), E < 200 MeV; analyzed cross sections and angular distributions. Compared results to ENDF/B6.
doi: 10.13182/NSE07-A2720
2007LI55 Nucl.Phys. A789, 103 (2007) Global triton optical model potential NUCLEAR REACTIONS 6,7Li, 9Be, 12,13C, 16O, 19F, 24,26Mg, 27Al, 27,28Si, 32S, 40,48Ca, 46,48Ti, 51V, 52Cr, 54,56Fe, 58,60,62,64Ni, 68Zn, 82Se, 87Rb, 86Sr, 89Y, 90,92,94,96Zr, 112,116,118,120,122,124Sn, 140Ce, 187W, 207,208Pb, 232Th(t, t'), E < 40 MeV; analyzed elastic scattering σ and angular distribution data to obtain a set of global optical model potential parameters. Compared results to other calculations.
doi: 10.1016/j.nuclphysa.2007.03.004
2006AN14 Phys.Rev. C 73, 054605 (2006) Global deuteron optical model potential for the energy range up to 183 MeV NUCLEAR REACTIONS 7Li, 12C, 14N, 16O, 24Mg, 27Al, 28Si, 32S, 40Ar, 40,48Ca, 48,49,50Ti, 50,51V, 52Cr, 54,56Fe, 59Co, 58,60,62,64Ni, 63,65Cu, 68Zn, 70,72Ge, 89Y, 90,91,92,94,96Zr, 93Nb, 100Mo, 103Rh, 105Pd, 112Cd, 115In, 112,116,120,124Sn, 140Ce, 165Ho, 181Ta, 197Au, 206,208Pb, 209Bi, 232Th, 238U(d, d), E ≈ 12-183 MeV; calculated σ(θ). Global optical potential, comparison with data.
doi: 10.1103/PhysRevC.73.054605
2006CA13 Nucl.Sci.Eng. 153, 93 (2006) MEND: A Program for Calculating the Complete Set of Nuclear Data of Medium-Heavy Nuclei in a Medium-Low Energy Region
doi: 10.13182/NSE05-06CCA
2005HA12 Nucl.Sci.Eng. 150, 78 (2005) Calculations and Evaluations of Cross sections for n + 204, 206, 207, 208, natPb Reactions in the En ≤ 250 MeV Energy Range NUCLEAR REACTIONS Pb, 204,206,207,208Pb(n, X), (n, n), (n, n'), (n, γ), (n, xn), (n, F), E ≤ 250 MeV; compiled, analyzed σ.
doi: 10.13182/NSE05-A2503
2005HA54 Nucl.Instrum.Methods Phys.Res. B239, 314 (2005) Y.Han, Z.Zhang, J.Chang, S.Oh, C.Cai Calculation and analysis of 63, 65, natCu(p, x) reaction cross sections in the Ep ≤ 250 MeV energy range NUCLEAR REACTIONS Cu, 63,65Cu(p, X), E ≈ 0-250 MeV; 63Cu(p, n), (p, 2n), (p, 3n), (p, np), (p, 2np), (p, 3np), (p, α), E ≈ 0-100 MeV; 65Cu(p, n), (p, 3n), (p, 4n), (p, 3np), (p, 4np), (p, α), E ≈ 0-100 MeV; Cu(p, X)62Zn/63Zn/65Zn/60Cu/61Cu/64Cu/56Co/57Co/58Co, E ≈ 0-250 MeV; calculated reaction σ. 63Cu(p, p), E=17.0, 30.3 MeV; calculated σ(θ). 63Cu(p, nX), (p, pX), (p, dX), (p, αX), E=50-250 MeV; calculated particle spectra. Comparison with data.
doi: 10.1016/j.nimb.2005.05.045
2004CA21 Nucl.Sci.Eng. 146, 221 (2004) Calculation of the Complete Sets of Nuclear Data for n + 92, 94, 96Mo below 20 MeV NUCLEAR REACTIONS 92,94,96Mo(n, X), (n, n), (n, n'), (n, γ), (n, p), (n, d), (n, α), E < 20 MeV; calculated σ, σ(θ). Comparisons with data.
doi: 10.13182/NSE04-A2405
2004TA36 Phys.Rev. C 70, 054306 (2004) Yu.-H.Tan, X.-H.Zhong, C.-H.Cai, P.-Z.Ning Effect of different baryon impurities NUCLEAR STRUCTURE 6Li, 10B, 12C, 16O, 40Ca, 208Pb; calculated binding energies, radii. 7Li, 11B, 13C, 17O, 41Ca, 209Pb; calculated hypernucleus binding energies, radii. Effects of different baryon impurities discussed.
doi: 10.1103/PhysRevC.70.054306
2003CA40 Nucl.Sci.Eng. 143, 301 (2003) Recalculation of Complete Sets of Nuclear Data for n + 85, 87Rb in Energy Region of 0.1 to 20 MeV NUCLEAR REACTIONS 85,87Rb(n, X), (n, γ), (n, n')(n, p), (n, α), (n, αX), (n, 2n), E=0.1-20 MeV; calculated σ. Comparison with data.
doi: 10.13182/NSE03-A2338
2003CA42 Europhys.Lett. 64, 448 (2003) C.H.Cai, L.Li, Y.H.Tan, P.Z.Ning Could Λ+c hypernuclei exist? NUCLEAR STRUCTURE 11B, 12,13C, 16O, 28Si, 32S, 40Ca, 51V, 89Y, 139La, 208Pb; calculated hypernucleus binding energies for Λ and Λc hyperons.
doi: 10.1209/epl/i2003-00610-x
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
2000TA22 Chin.Phys.Lett. 17, 401 (2000) Yu-H.Tan, Y.-A.Luo, P.-Z.Ning, C.-H.Cai Shell Model Analysis of Ξ- Hypernuclei Spectra for Mass A = 12 and A = 16 NUCLEAR STRUCTURE 12Be, 16C; calculated hypernuclei binding and single particle energies, level, J, π. Effect of residual interaction investigated.
1998LI38 Nucl.Phys. A639, 493c (1998) Uncoventional Medium Effect in K+-Nucleus Scattering NUCLEAR REACTIONS 6Li, C, Si, Ca(K+, X), E at 400-800 MeV/c; calculated total σ; deduced unconventional medium effect. 12C, 40Ca(K+, K+), E at 800 MeV/c; 12C, 6Li(K+, K+), E at 715 MeV/c; calculated σ(θ). Comparisons with data.
doi: 10.1016/S0375-9474(98)00316-9
1996CA45 Chin.J.Nucl.Phys. 18, No 1, 1 (1996) On the Relativistic Schrodinger Equation of Meson-Nucleus Scattering NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, K+), E at 400-800 MeV/c; analyzed σ(θ), σ; deduced model parameters. Relativistic Schrodinger equation, target recoil, medium effects.
1996SH11 Chin.Phys.Lett. 13, 343 (1996) H.Shen, P.-Z.Ning, C.-H.Cai, H.-Y.Wang On the A -Dependence of the Okamoto-Nolen-Schiffer Anomaly NUCLEAR STRUCTURE A ≤ 40; analyzed mirror nuclei mass differences; deduced Okamoto-Nolen-Schiffer anomaly related features.
doi: 10.1088/0256-307X/13/5/007
1995CA44 Chin.J.Nucl.Phys. 17, No 2, 95 (1995) C.H.Cai, P.Z.Ning, H.Shen, Z.M.Xue, S.Y.Yu Unconventional Medium Effect in K+ Scattering from 6Li, 12C, 28Si and 40Ca NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, K+), E at 400-800 MeV/c; analyzed σ(θ), σ ratio. Quark NJL model.
1995SH46 Chin.J.Nucl.Phys. 17, No 2, 102 (1995) H.Shen, P.-Z.Ning, C.-H.Cai, L.-C.Xiang Influence of the In-Medium Nucleon Swelling on Pion-Nucleus Scattering at High Energy NUCLEAR REACTIONS 12C(K+, K+), E at 800 MeV/c; analyzed σ(θ); deduced nucleon swelling evidence. Optical model.
1991CA21 Nucl.Sci.Eng. 109, 142 (1991) Comparisons of Global Phenomenological and Microscopic Optical Potentials for Nuclear Data Predictions NUCLEAR REACTIONS 59Co(n, n), (n, n'), E ≤ 20 MeV; calculated σ(E). 59Co(n, n), E=2.47, 8 MeV; calculated σ(θ). 98Mo(n, p), (n, nα), (n, γ), (n, np), (n, α), E=threshold-20 MeV; 100Mo(n, 2n), E ≈ 8.5-20 MeV; calculated σ(E). Optical model from other data analysis.
doi: 10.13182/NSE91-A28513
1991CA26 Chin.J.Nucl.Phys. 13, No 1, 45 (1991) C.Cai, D.Liu, Q.Shen, Y.Tian, Y.Zhuo Comparison between Phenomenological and Microscopic Optical Potential in Nuclear Data Evaluations NUCLEAR REACTIONS 27Al, 31P, S, Cl, K, Ca, Fe, 59Co, Cu, Ag, In, Sb, W, Pb(n, n), E ≈ 0.083-24 MeV; calculated σ. Comparison with data. Different models chi square fits, phenomenological optimal, global and microscopic optical potentials.
1988TI04 Chin.J.Nucl.Phys. 10, 183 (1988) Tian Ye, Han Yinlu, Shen Qingbiao, Cai Chonghai Calculation and Analysis of Fast Neutron Cross Sections on Mo with Microscopic Optical Potential NUCLEAR REACTIONS 98Mo(n, p), (n, γ), (n, α), (n, np), 100Mo(n, 2n), E=threshold-20 MeV; calculated σ(E). 98Mo(n, n), E=0.5-26 MeV; calculated σ(θ). Hauser-Feshbach, preequilibrium exciton (with evaporation) models, microscopic optical potential.
1988YU04 Phys.Rev. C38, 272 (1988) Yu Zi-qiang, Cai Chong-hai, Ma Wei-hsing, Zhao Shu-ping Contribution of the Second Kind of Meson Exchange Current to Pion-Nucleus Double-Charge-Exchange Reactions 18O(π+, π-)18Ne(g.s.) and 14C(π+, π-)14O(g.s.) NUCLEAR REACTIONS 14C, 18O(π+, π-), E=164, 292 MeV; calculated σ(θ); deduced meson exchange current features.
doi: 10.1103/PhysRevC.38.272
1984HE21 Chin.J.Nucl.Phys. 6, 234 (1984) Microscopic Theory for Nucleon-Nucleus Optical Potential in Intermediate Energies NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated nucleon-nucleus potential. Microscopic model.
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