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ß-Delayed One and Two Neutron Emission Probabilities Southeast of
Phong, V H; Nishimura, S; Lorusso, G; Davinson, T; Estrade, A; Hall, O; Kawano, T; Liu, J; Montes, F; Nishimura, N; Grzywacz, R; Rykaczewski, K P; Agramunt, J; Ahn, D S; Algora, A; Allmond, J M; Baba, H; Bae, S; Brewer, N T; Bruno, C G; Caballero-Folch, R; Calviño, F; Coleman-Smith, P J; Cortes, G; Dillmann, I; Domingo-Pardo, C; Fijalkowska, A; Fukuda, N; Go, S; Griffin, C J; Ha, J; Harkness-Brennan, L J; Isobe, T; Kahl, D; Khiem, L H; Kiss, G G; Korgul, A; Kubono, S; Labiche, M; Lazarus, I; Liang, J; Liu, Z; Matsui, K; Miernik, K; Moon, B; Morales, A I; Morrall, P; Nepal, N; Page, R D; Piersa-Silkowska, M.
Afiliação
  • Phong VH; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Nishimura S; University of Science, Vietnam National University, Hanoi 120062, Vietnam.
  • Lorusso G; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Davinson T; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Estrade A; National Physical Laboratory, Teddington TW11 0LW, United Kingdom.
  • Hall O; Department of Physics, University of Surrey, Guildford GU2 7XH, United Kingdom.
  • Kawano T; School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
  • Liu J; Department of Physics, Central Michigan University, Mount Pleasant, Michigan 48859, USA.
  • Montes F; School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
  • Nishimura N; Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Grzywacz R; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Rykaczewski KP; Department of Physics, University of Hong Kong, Pokfulman Road, Hong Kong.
  • Agramunt J; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Ahn DS; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Algora A; Astrophysical Big-Bang Laboratory, Cluster for Pioneering Research, RIKEN, Wako, Saitama 351-0198, Japan.
  • Allmond JM; Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA.
  • Baba H; Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
  • Bae S; Instituto de Fsica Corpuscular, CSIC and Universitat de Valencia, E-46980 Paterna, Spain.
  • Brewer NT; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Bruno CG; Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon 34126, Republic of Korea.
  • Caballero-Folch R; Instituto de Fsica Corpuscular, CSIC and Universitat de Valencia, E-46980 Paterna, Spain.
  • Calviño F; Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
  • Coleman-Smith PJ; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Cortes G; Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon 34126, Republic of Korea.
  • Dillmann I; Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA.
  • Domingo-Pardo C; Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
  • Fijalkowska A; School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
  • Fukuda N; TRIUMF, Vancouver, British Columbia V6T 2A3, Canada.
  • Go S; Universitat Politecnica de Catalunya, E-08028 Barcelona, Spain.
  • Griffin CJ; STFC Daresbury Laboratory, Daresbury, Warrington WA4 4AD, United Kingdom.
  • Ha J; Universitat Politecnica de Catalunya, E-08028 Barcelona, Spain.
  • Harkness-Brennan LJ; TRIUMF, Vancouver, British Columbia V6T 2A3, Canada.
  • Isobe T; Department of Physics and Astronomy, University of Victoria, Victoria, British Columbia V8P 5C2, Canada.
  • Kahl D; Instituto de Fsica Corpuscular, CSIC and Universitat de Valencia, E-46980 Paterna, Spain.
  • Khiem LH; Faculty of Physics, University of Warsaw, PL02-093 Warsaw, Poland.
  • Kiss GG; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Korgul A; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Kubono S; School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
  • Labiche M; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Lazarus I; Seoul National University, Department of Physics and Astronomy, Seoul 08826, Republic of Korea.
  • Liang J; Department of Physics, University of Liverpool, Liverpool L69 7ZE, United Kingdom.
  • Liu Z; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Matsui K; School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
  • Miernik K; Extreme Light Infrastructure-Nuclear Physics, Horia Hulubei National Institute for R&D in Physics and Nuclear Engineering (IFIN-HH), 077125 Bucharest-Magurele, Romania.
  • Moon B; Institute of Physics, Vietnam Academy of Science and Technology, Ba Dinh, 118011 Hanoi, Vietnam.
  • Morales AI; Graduate University of Science and Technology, Vietnam Academy of Science and Technology, Cau Giay, 122102 Hanoi, Vietnam.
  • Morrall P; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
  • Nepal N; Institute for Nuclear Research (Atomki), Debrecen H4032, Hungary.
  • Page RD; Faculty of Physics, University of Warsaw, PL02-093 Warsaw, Poland.
  • Piersa-Silkowska M; RIKEN Nishina Center, Wako, Saitama 351-0198, Japan.
Phys Rev Lett ; 129(17): 172701, 2022 Oct 21.
Article em En | MEDLINE | ID: mdl-36332266
ABSTRACT
The ß-delayed one- and two-neutron emission probabilities (P_{1n} and P_{2n}) of 20 neutron-rich nuclei with N≥82 have been measured at the RIBF facility of the RIKEN Nishina Center. P_{1n} of ^{130,131}Ag, ^{133,134}Cd, ^{135,136}In, and ^{138,139}Sn were determined for the first time, and stringent upper limits were placed on P_{2n} for nearly all cases. ß-delayed two-neutron emission (ß2n) was unambiguously identified in ^{133}Cd and ^{135,136}In, and their P_{2n} were measured. Weak ß2n was also detected from ^{137,138}Sn. Our results highlight the effect of the N=82 and Z=50 shell closures on ß-delayed neutron emission probability and provide stringent benchmarks for newly developed macroscopic-microscopic and self-consistent global models with the inclusion of a statistical treatment of neutron and γ emission. The impact of our measurements on r-process nucleosynthesis was studied in a neutron star merger scenario. Our P_{1n} and P_{2n} have a direct impact on the odd-even staggering of the final abundance, improving the agreement between calculated and observed Solar System abundances. The odd isotope fraction of Ba in r-process-enhanced (r-II) stars is also better reproduced using our new data.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article