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Mass Measurement of Upper fp-Shell N=Z-2 and N=Z-1 Nuclei and the Importance of Three-Nucleon Force along the N=Z Line.
Wang, M; Zhang, Y H; Zhou, X; Zhou, X H; Xu, H S; Liu, M L; Li, J G; Niu, Y F; Huang, W J; Yuan, Q; Zhang, S; Xu, F R; Litvinov, Yu A; Blaum, K; Meisel, Z; Casten, R F; Cakirli, R B; Chen, R J; Deng, H Y; Fu, C Y; Ge, W W; Li, H F; Liao, T; Litvinov, S A; Shuai, P; Shi, J Y; Song, Y N; Sun, M Z; Wang, Q; Xing, Y M; Xu, X; Yan, X L; Yang, J C; Yuan, Y J; Zeng, Q; Zhang, M.
Afiliação
  • Wang M; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Zhang YH; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Zhou X; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Zhou XH; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Xu HS; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Liu ML; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Li JG; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Niu YF; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Huang WJ; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Yuan Q; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Zhang S; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Xu FR; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Litvinov YA; School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China.
  • Blaum K; Frontiers Science Center for Rare isotope, Lanzhou University, Lanzhou 730000, China.
  • Meisel Z; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Casten RF; Advanced Energy Science and Technology Guangdong Laboratory, Huizhou, 516007, China.
  • Cakirli RB; State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, People's Republic of China.
  • Chen RJ; State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, People's Republic of China.
  • Deng HY; State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, People's Republic of China.
  • Fu CY; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Ge WW; GSI Helmholtzzentrum für Schwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany.
  • Li HF; Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany.
  • Liao T; Institute of Nuclear and Particle Physics, Department of Physics and Astronomy, Ohio University, Athens, Ohio 45701, USA.
  • Litvinov SA; Wright Nuclear Structure Laboratory, Yale University, New Haven, Connecticut 06520-8124, USA.
  • Shuai P; Department of Physics, Istanbul University, Istanbul 34134, Turkey.
  • Shi JY; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Song YN; GSI Helmholtzzentrum für Schwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany.
  • Sun MZ; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Wang Q; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Xing YM; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Xu X; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Yan XL; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Yang JC; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Yuan YJ; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Zeng Q; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.
  • Zhang M; CAS Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
Phys Rev Lett ; 130(19): 192501, 2023 May 12.
Article em En | MEDLINE | ID: mdl-37243656
ABSTRACT
Using a novel method of isochronous mass spectrometry, the masses of ^{62}Ge, ^{64}As, ^{66}Se, and ^{70}Kr are measured for the first time, and the masses of ^{58}Zn, ^{61}Ga, ^{63}Ge, ^{65}As, ^{67}Se, ^{71}Kr, and ^{75}Sr are redetermined with improved accuracy. The new masses allow us to derive residual proton-neutron interactions (δV_{pn}) in the N=Z nuclei, which are found to decrease (increase) with increasing mass A for even-even (odd-odd) nuclei beyond Z=28. This bifurcation of δV_{pn} cannot be reproduced by the available mass models, nor is it consistent with expectations of a pseudo-SU(4) symmetry restoration in the fp shell. We performed ab initio calculations with a chiral three-nucleon force (3NF) included, which indicate the enhancement of the T=1 pn pairing over the T=0 pn pairing in this mass region, leading to the opposite evolving trends of δV_{pn} in even-even and odd-odd nuclei.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2023 Tipo de documento: Article