A collective coupled-channel model and mirror state energy displacements

被引:5
|
作者
Fraser, P. R. [1 ]
Amos, K. [2 ,3 ]
Canton, L. [4 ]
Karataglidis, S. [2 ,3 ]
van der Knijff, D. [2 ]
Svenne, J. P. [5 ,6 ]
机构
[1] Curtin Univ, Inst Theoret Phys, Bentley, WA 6102, Australia
[2] Univ Melbourne, Sch Phys, Melbourne, Vic 3010, Australia
[3] Univ Johannesburg, Dept Phys, ZA-2006 Johannesburg, South Africa
[4] Ist Nazl Fis Nucl, Sez Padova, I-35131 Padua, Italy
[5] Univ Manitoba, Dept Phys & Astron, Winnipeg, MB R3T 2N2, Canada
[6] Winnipeg Inst Theoret Phys, Winnipeg, MB R3T 2N2, Canada
来源
EUROPEAN PHYSICAL JOURNAL A | 2015年 / 51卷 / 09期
基金
新加坡国家研究基金会;
关键词
COULOMB ENERGY; SCATTERING; NUCLEI; F-15;
D O I
10.1140/epja/i2015-15110-4
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The spectra of nucleon-nucleus mirror systems allow examination of charge symmetry breaking in nucleon-nucleus interactions. To date, such examination has been performed with studies using microscopic models of structure. Herein we seek characterisation with a coupled-channel model in which the nucleon-nucleus interactions are described using a collective model prescription with the Pauli principle taken into account. The neutron-nucleus Hamiltonian is chosen to give the best match to the compound system spectrum, with emphasis on finding the correct ground state energy relative to the neutron-nucleus threshold. The Coulomb interactions for the proton-nucleus partner of a mirror pair are determined using charge distributions that match the root-mean-square charge radii of the nuclei in question. With the Coulomb interaction so defined modifying the neutron-nucleus Hamiltonian, we then predict a spectrum for the relevant proton-nucleus compound. Discrepancies in that resulting spectrum with measured values we tentatively ascribe to charge-symmetry breaking effects. We consider spectra obtained in this way for the mirror pairs C-13 and N-13, C-15 and F-15, and O-15 and N-15, all to similar to 10 MeV excitation.
引用
收藏
页数:14
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