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First Application of Mass Measurements with the Rare-RI Ring Reveals the Solar r-Process Abundance Trend at A=122 and A=123.
Li, H F; Naimi, S; Sprouse, T M; Mumpower, M R; Abe, Y; Yamaguchi, Y; Nagae, D; Suzaki, F; Wakasugi, M; Arakawa, H; Dou, W B; Hamakawa, D; Hosoi, S; Inada, Y; Kajiki, D; Kobayashi, T; Sakaue, M; Yokoda, Y; Yamaguchi, T; Kagesawa, R; Kamioka, D; Moriguchi, T; Mukai, M; Ozawa, A; Ota, S; Kitamura, N; Masuoka, S; Michimasa, S; Baba, H; Fukuda, N; Shimizu, Y; Suzuki, H; Takeda, H; Ahn, D S; Wang, M; Fu, C Y; Wang, Q; Suzuki, S; Ge, Z; Litvinov, Yu A; Lorusso, G; Walker, P M; Podolyak, Zs; Uesaka, T.
Afiliação
  • Li HF; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China.
  • Naimi S; Lanzhou University, Lanzhou 730000, People's Republic of China.
  • Sprouse TM; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Mumpower MR; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Abe Y; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Yamaguchi Y; Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Nagae D; Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Suzaki F; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Wakasugi M; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Arakawa H; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Dou WB; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Hamakawa D; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Hosoi S; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Inada Y; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Kajiki D; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Kobayashi T; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Sakaue M; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Yokoda Y; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Yamaguchi T; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Kagesawa R; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Kamioka D; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Moriguchi T; Department of Physics, Saitama University, Saitama 338-8570, Japan.
  • Mukai M; Institute of Physics, University of Tsukuba, Ibaraki 305-8571, Japan.
  • Ozawa A; Institute of Physics, University of Tsukuba, Ibaraki 305-8571, Japan.
  • Ota S; Institute of Physics, University of Tsukuba, Ibaraki 305-8571, Japan.
  • Kitamura N; Institute of Physics, University of Tsukuba, Ibaraki 305-8571, Japan.
  • Masuoka S; Institute of Physics, University of Tsukuba, Ibaraki 305-8571, Japan.
  • Michimasa S; Center for Nuclear Study, University of Tokyo, Wako, Saitama 351-0198, Japan.
  • Baba H; Center for Nuclear Study, University of Tokyo, Wako, Saitama 351-0198, Japan.
  • Fukuda N; Center for Nuclear Study, University of Tokyo, Wako, Saitama 351-0198, Japan.
  • Shimizu Y; Center for Nuclear Study, University of Tokyo, Wako, Saitama 351-0198, Japan.
  • Suzuki H; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Takeda H; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Ahn DS; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Wang M; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Fu CY; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Wang Q; Riken Nishina Center for Accelerator-Based Science, Wako, Saitama 351-0198, Japan.
  • Suzuki S; Center for Exotic Nuclear Studies, Institute for Basic Science (IBS), Daejeon 34126, Republic of Korea.
  • Ge Z; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China.
  • Litvinov YA; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China.
  • Lorusso G; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China.
  • Walker PM; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China.
  • Podolyak Z; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, People's Republic of China.
  • Uesaka T; GSI Helmholtzzentrum für Schwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany.
Phys Rev Lett ; 128(15): 152701, 2022 Apr 15.
Article em En | MEDLINE | ID: mdl-35499908
ABSTRACT
The Rare-RI Ring (R3) is a recently commissioned cyclotronlike storage ring mass spectrometer dedicated to mass measurements of exotic nuclei far from stability at Radioactive Isotope Beam Factory (RIBF) in RIKEN. The first application of mass measurement using the R3 mass spectrometer at RIBF is reported. Rare isotopes produced at RIBF-^{127}Sn, ^{126}In, ^{125}Cd, ^{124}Ag, ^{123}Pd-were injected in R3. Masses of ^{126}In, ^{125}Cd, and ^{123}Pd were measured whereby the mass uncertainty of ^{123}Pd was improved. This is the first reported measurement with a new storage ring mass spectrometry technique realized at a heavy-ion cyclotron and employing individual injection of the preidentified rare nuclei. The latter is essential for the future mass measurements of the rarest isotopes produced at RIBF. The impact of the new ^{123}Pd result on the solar r-process abundances in a neutron star merger event is investigated by performing reaction network calculations of 20 trajectories with varying electron fraction Y_{e}. It is found that the neutron capture cross section on ^{123}Pd increases by a factor of 2.2 and ß-delayed neutron emission probability, P_{1 n}, of ^{123}Rh increases by 14%. The neutron capture cross section on ^{122}Pd decreases by a factor of 2.6 leading to pileup of material at A=122, thus reproducing the trend of the solar r-process abundances. The trend of the two-neutron separation energies (S_{2n}) was investigated for the Pd isotopic chain. The new mass measurement with improved uncertainty excludes large changes of the S_{2n} value at N=77. Such large increase of the S_{2n} values before N=82 was proposed as an alternative to the quenching of the N=82 shell gap to reproduce r-process abundances in the mass region of A=112-124.

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

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