NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of May 3, 2024.

Search: Author = Cai Chong-hai

Found 41 matches.

Back to query form

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 T_1/2. 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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, 245}Pu 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2016SU02      Ann.Nucl.Energy 90, 123 (2016)

X.Su, Y.Han, C.Cai

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
Citations: PlumX Metrics

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(E_out). ²⁷Al(n, ³He), E=95.6 MeV; calculated σ(E_out, θ). ²⁰⁹Bi(p, 3n), (p, 2np), E=20-200 MeV; calculated σ. ²⁰⁹Bi(p, x), E=61.7 MeV; calculated σ(E_out, θ). UNF code (optical model plus unified HF plus exciton model); compared with data.

doi: 10.1016/j.nds.2014.04.012
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2014SU19      Ann.Nucl.Energy 76, 469 (2014)

X.Su, Y.Han, C.Cai

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
Citations: PlumX Metrics

2013HA04      Ann.Nucl.Energy 55, 75 (2013)

Y.Han, Y.Xu, C.Cai, Q.Shen

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2011HA46      J.Korean Phys.Soc. 59, 1069s (2011)

Y.Han, Q.Shen, C.Cai, Z.Zhang

Present Status of Evaluated Nuclear Data Library for Accelerator-Driven Systems in China

COMPILATION ^24,25,26Mg, ²⁷Al, ^28,29,30Si, ^{40,42,43,44,46,48}Ca, ^50,52,53,54Cr, ^54,56,57,58Fe, ⁵⁹Co, ^{58,60,61,62,64}Ni, ^63,65Cu, ^{90,91,92,94,96}Zr, ⁹³Nb, ^{91,94,95,96,97,98,100}Mo, ^{180,182,183,184,186}W, ^{204,206,207,208}Pb, ²⁰⁹Bi, ²³²Th, ²³⁷Np, ^{232,233,234,235,236,237,238,239,240}U, ^{236,244,245,245}Pu, ^{241,242m,242,243}Am, ^{243,244,245,246,247,248}Cm(n, X), (p, X), E=0-200 MeV; calculated, evaluated σ, σ(E, θ).

doi: 10.3938/jkps.59.1069
Citations: PlumX Metrics

2010CA03      Nucl.Sci.Eng. 164, 304 (2010)

C.Cai, K.Xu, H.An, H.Wu

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
Citations: PlumX Metrics

2010HA01      Nucl.Sci.Eng. 164, 185 (2010)

Y.Han, P.Liu, C.Cai

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2010ZH02      Ann.Nucl.Energy 37, 130 (2010)

Z.Zhang, Y.Han, C.Cai

Double differential cross sections of light charged particle emission in neutron induced reactions on ^{54, 56, 57, 58}Fe

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
Citations: PlumX Metrics

2009LI09      Eur.Phys.J. A 39, 255 (2009)

X.Li, H.An, C.Cai

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, ^{58,60,61,62,64}Ni, ^63,65Cu, ⁶⁸Zn, ⁷⁴Ge, ⁸⁶Sr, ⁸⁹Y, ^{90,91,92,94,96}Zr, ⁹³Nb, ^92,100Mo, ¹⁰³Rh, ¹⁰⁵Pd, ¹¹²Cd, ¹¹⁵In, ^{112,116,118,120,124}Sn, 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
Citations: PlumX Metrics

2008HA33      Ann.Nucl.Energy 35, 2031 (2008)

Y.Han, Y.Zhang, H.Guo, C.Cai

Double differential cross sections of neutron and proton emission in neutron induced reactions on ^{54, 56, 57, 58}Fe

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
Citations: PlumX Metrics

2008LI05      Nucl.Phys. A801, 43 (2008)

X.Li, C.Cai

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, ^{74,76,78,80,82}Se, ^86,88Sr, ⁸⁹Y, ^{90,91,92,94,96}Zr, ^{92,94,96,98,100}Mo, ¹⁰²Ru, ^{104,106,108,110}Pd, ^{106,108,110,111,112,113,114,116}Cd, ^116,120,124Sn, ^134,136,138Ba, ¹⁴⁴Nd, ^{144,148,150,152,154}Sm, 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). ^{112,114,116,118,120,122,124}Sn(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
Citations: PlumX Metrics

2007LI55      Nucl.Phys. A789, 103 (2007)

X.Li, C.Liang, C.Cai

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, ^{112,116,118,120,122,124}Sn, 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
Citations: PlumX Metrics

2006AN14      Phys.Rev. C 73, 054605 (2006)

H.An, C.Cai

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, ^{90,91,92,94,96}Zr, ⁹³Nb, ¹⁰⁰Mo, ¹⁰³Rh, ¹⁰⁵Pd, ¹¹²Cd, ¹¹⁵In, ^{112,116,120,124}Sn, 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
Citations: PlumX Metrics

2005HA12      Nucl.Sci.Eng. 150, 78 (2005)

Y.Han, Q.Shen, Z.Zhang, C.Cai

Calculations and Evaluations of Cross sections for n + ^{204, 206, 207, 208, nat}Pb Reactions in the E_n ≤ 250 MeV Energy Range

NUCLEAR REACTIONS Pb, ^{204,206,207,208}Pb(n, X), (n, n), (n, n'), (n, γ), (n, xn), (n, F), E ≤ 250 MeV; compiled, analyzed σ.

doi: 10.13182/NSE05-A2503
Citations: PlumX Metrics

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, nat}Cu(p, x) reaction cross sections in the E_p ≤ 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
Citations: PlumX Metrics

2004CA21      Nucl.Sci.Eng. 146, 221 (2004)

C.Cai

Calculation of the Complete Sets of Nuclear Data for n + ^{92, 94, 96}Mo 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
Citations: PlumX Metrics

2003CA40      Nucl.Sci.Eng. 143, 301 (2003)

C.Cai

Recalculation of Complete Sets of Nuclear Data for n + ^{85, 87}Rb 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1998LI38      Nucl.Phys. A639, 493c (1998)

L.Li, C.Cai, P.Ning

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
Citations: PlumX Metrics

1996CA45      Chin.J.Nucl.Phys. 18, No 1, 1 (1996)

C.Cai, H.Shen, P.Ning

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.

1991CA21      Nucl.Sci.Eng. 109, 142 (1991)

C.Cai, Q.Shen, Y.Zhuo

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1984HE21      Chin.J.Nucl.Phys. 6, 234 (1984)

He Guozhu, Cai Chonghai

Microscopic Theory for Nucleon-Nucleus Optical Potential in Intermediate Energies

NUCLEAR STRUCTURE ⁴He, ¹⁶O, ⁴⁰Ca; calculated nucleon-nucleus potential. Microscopic model.