dorsal/arxiv
View SchemaAntisymmetrization of a Mean Field Calculation of the T-Matrix
| Authors | A. Wierling, B. G. Giraud, F. Mekideche, H. Horiuchi, T. Maruyama, A. Ohnishi, J. C. Lemm, A. Weiguny |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9402002 |
| URL | https://arxiv.org/abs/nucl-th/9402002 |
| DOI | 10.1007/BF01291912 |
| Journal | Z.Phys. A348 (1994) 153-168 |
Abstract
The usual definition of the prior(post) interaction $V(V^\prime )$ between projectile and target (resp. ejectile and residual target) being contradictory with full antisymmetrization between nucleons, an explicit antisymmetrization projector ${\cal A}$ must be included in the definition of the transition operator, $ T\equiv V^\prime{\cal A}+V^\prime{\cal A}GV. $ We derive the suitably antisymmetrized mean field equations leading to a non perturbative estimate of $T$. The theory is illustrated by a calculation of forward $\alpha$-$\alpha$ scattering, making use of self consistent symmetries.
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"abstract": "The usual definition of the prior(post) interaction $V(V^\\prime )$ between\nprojectile and target (resp. ejectile and residual target) being contradictory\nwith full antisymmetrization between nucleons, an explicit antisymmetrization\nprojector ${\\cal A}$ must be included in the definition of the transition\noperator, $ T\\equiv V^\\prime{\\cal A}+V^\\prime{\\cal A}GV. $ We derive the\nsuitably antisymmetrized mean field equations leading to a non perturbative\nestimate of $T$. The theory is illustrated by a calculation of forward\n$\\alpha$-$\\alpha$ scattering, making use of self consistent symmetries.",
"arxiv_id": "nucl-th/9402002",
"authors": [
"A. Wierling",
"B. G. Giraud",
"F. Mekideche",
"H. Horiuchi",
"T. Maruyama",
"A. Ohnishi",
"J. C. Lemm",
"A. Weiguny"
],
"categories": [
"nucl-th"
],
"doi": "10.1007/BF01291912",
"journal_ref": "Z.Phys. A348 (1994) 153-168",
"title": "Antisymmetrization of a Mean Field Calculation of the T-Matrix",
"url": "https://arxiv.org/abs/nucl-th/9402002"
},
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