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Multi-guasiparticle excitations of 91Ru

Multi-guasiparticle excitations of 91Ru
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摘要 The level structure in neutron-deficient nucleus 91Ru was investigated via the 58Ni(36Ar,2 plnγ)Ru reaction at a beam energy of 111 MeV.Charged particles,neutrons,and y-rays were emitted in this reaction and detected by the DIAMANT CsI ball,Neutron Wall,and the EXOGAM Ge clover array,respectively.In addition to the previously reported levels in 91Ru,new low-to-medium spin states were observed.Angular correlation and linear polarization measurements were performed to unambiguously determine spins and parities of the excited states in 91 Ru.The low-spin states of 91 Ru exhibit a scheme of multi-quasiparticle excitations,which is very similar to that of the neighboring N=47 isotone.These excitations have been interpreted in terms of the shell model.The calculations performed in the configuration space(p3/2,f5/2,p1/2,g9/2)reproduce the experimental excitation energies reasonably well,supporting the interpretation of the newly assigned positive-parity states in terms of the three quasiparticle configurationsπ(g9/2)^-2v(g9/2^-1 and v(g9/2)^-3. The level structure in neutron-deficient nucleus 91Ru was investigated via the 58Ni(36Ar,2 plnγ) Ru reaction at a beam energy of 111 MeV.Charged particles,neutrons,and y-rays were emitted in this reaction and detected by the DIAMANT CsI ball,Neutron Wall,and the EXOGAM Ge clover array,respectively.In addition to the previously reported levels in 91Ru,new low-to-medium spin states were observed.Angular correlation and linear polarization measurements were performed to unambiguously determine spins and parities of the excited states in 91 Ru.The low-spin states of 91 Ru exhibit a scheme of multi-quasiparticle excitations,which is very similar to that of the neighboring N=47 isotone.These excitations have been interpreted in terms of the shell model.The calculations performed in the configuration space(p3/2,f5/2,p1/2,g9/2) reproduce the experimental excitation energies reasonably well,supporting the interpretation of the newly assigned positive-parity states in terms of the three quasiparticle configurations π(g9/2)-2v(g9/2-1 and v(g9/2)-3.
作者 郑勇 Gde France 周小红 黄山 柳敏良 Yong Zheng;Gde France;Xiao-Hong Zhou;Shan Huang;Min-Liang Liu(Institute of Modern Physics,Chinese Academy of Sciences,Lanzhou 730000,China;Grand Accélérateur National d’Ions Lourds(GANIL),CEA/DSM-CNRS/IN2P3,Bd Henri Becquerel,BP 55027,F-14076 Caen Cedex5,France)
出处 《Chinese Physics C》 SCIE CAS CSCD 2020年第2期80-87,共8页 中国物理C(英文版)
基金 Supported by National Natural Science Foundation of China(U1632137)
关键词 level structure neutron deficient nucleus low-spin states shell model three quasiparticle configuration level structure neutron deficient nucleus low-spin states shell model three quasiparticle configuration
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