Isospin structure of Jπ=1+ states in Ni58 and Cu58 studied by Ni58(p,p') and Ni58(He3,t)Cu58 measurements

Isospin structure of Jπ=1+ states in Ni58 and Cu58 studied by Ni58(p,p') and Ni58(He3,t)Cu58 measurements
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通过 Ni58(p,p) 和 Ni58(He3,t)Cu58 测量研究 Ni58 和 Cu58 中 Jπ=1+ 态的同位旋结构

DOI:
10.1103/physrevc.75.034310
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发表时间:
2007
期刊:
影响因子:
3.1
通讯作者:
M. Yosoi
M. Yosoi
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
H. Fujita;Y. Fujita;T. Adachi;A. Bacher;G. Berg;T. Black;E. Caurier;C. Foster;H. Fujimura;K. Hara;K. Harada;K. Hatanaka;J. Jänecke;J. Kamiya;Y. Kanzaki;K. Katori;T. Kawabata;K. Langanke;G. Martínez;T. Noro;D. Roberts;H. Sakaguchi;Y. Shimbara;T. Shinada;E. Stephenson;H. Ueno;T. Yamanaka;M. Yoshifuku;M. Yosoi

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Isospin is a good quantum number under the assumption that the nuclear interaction is charge independent. An analogous structure of excited states is expected for nuclei with the same mass numberbut with differentcomponentsof the isospin, where. The analogous structure has been studied for the isobaric nucleiandby comparing the transitions from theground state (initial isospinand) to theand the Gamow-Teller (GT) states () inand, respectively. For this purpose, proton inelastic scattering () atMeV and the charge-exchange (,) reaction at 140 MeV/nucleon were both measured at, exciting final states with isospinand 2 and, 1, and 2, respectively. High energy and scattering-angle resolutions were achieved by applying complete beam matching techniques. On the basis of the correspondence between excitation energies and transition strengths, isospin valuesand 2 of analog GT andstates were identified. The distribution ofstates was also compared with results of(),(), and() experiments, in which onlystates are excited. The obtained GT strength distribution is compared with the results of shell-model calculations.