dorsal/arxiv
View SchemaMicroscopic analysis of T=1 and T=0 proton-neutron correlations in $N=Z$ nuclei
| Authors | M. Hasegawa, K. Kaneko |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/0411037 |
| URL | https://arxiv.org/abs/nucl-th/0411037 |
| DOI | 10.1016/j.nuclphysa.2004.11.014 |
| Journal | Nucl.Phys. A748 (2005) 393-401 |
Abstract
The competition between the isovector (T=1) and isoscalar (T=0) proton-neutron ($p-n$) correlations in $N=Z$ nuclei is investigated by calculating their correlation energies with a realistic effective interaction which reproduces observed nuclear properties very well, in a strict shell model treatment. It is shown in the realistic shell model that the double-differences of binding energies $(B(A+pn:T) + B(A) - B(A+p) - B(A+n))$ ($B(A)$ being the binding energy) are good indicators of the T=1 and T=0 $p-n$ correlations. Each of them, however, originates in plural kinds of correlations with T=1 or T=0.
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"abstract": "The competition between the isovector (T=1) and isoscalar (T=0)\nproton-neutron ($p-n$) correlations in $N=Z$ nuclei is investigated by\ncalculating their correlation energies with a realistic effective interaction\nwhich reproduces observed nuclear properties very well, in a strict shell model\ntreatment. It is shown in the realistic shell model that the double-differences\nof binding energies $(B(A+pn:T) + B(A) - B(A+p) - B(A+n))$ ($B(A)$ being the\nbinding energy) are good indicators of the T=1 and T=0 $p-n$ correlations. Each\nof them, however, originates in plural kinds of correlations with T=1 or T=0.",
"arxiv_id": "nucl-th/0411037",
"authors": [
"M. Hasegawa",
"K. Kaneko"
],
"categories": [
"nucl-th"
],
"doi": "10.1016/j.nuclphysa.2004.11.014",
"journal_ref": "Nucl.Phys. A748 (2005) 393-401",
"title": "Microscopic analysis of T=1 and T=0 proton-neutron correlations in $N=Z$ nuclei",
"url": "https://arxiv.org/abs/nucl-th/0411037"
},
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