dorsal/arxiv
View SchemaTheory of Coupled Pion--Trinucleon Systems
| Authors | L. Canton, G. Cattapan |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9312016 |
| URL | https://arxiv.org/abs/nucl-th/9312016 |
| DOI | 10.1103/PhysRevC.50.2761 |
| Journal | Phys.Rev.C50:2761-2767,1994 |
Abstract
We derive the dynamical equations which consistently couple the four--body ($\pi$NNN) system to the underlying three--nucleon system. Our treatment can be considered the proper generalization of the Afnan--Blankleider equations for the coupled NN--$\pi$NN system. The resulting connected--kernel equation resembles in structure the Yakubovskii--Grassberger--Sandhas equation for the standard four--body problem, but involves 24 chain--labelled components (rather than the usual 18 ones) and allows for a consistent evaluation of reaction amplitudes involving $\pi$ absorption/production.
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"abstract": "We derive the dynamical equations which consistently couple the four--body\n($\\pi$NNN) system to the underlying three--nucleon system. Our treatment can be\nconsidered the proper generalization of the Afnan--Blankleider equations for\nthe coupled NN--$\\pi$NN system. The resulting connected--kernel equation\nresembles in structure the Yakubovskii--Grassberger--Sandhas equation for the\nstandard four--body problem, but involves 24 chain--labelled components (rather\nthan the usual 18 ones) and allows for a consistent evaluation of reaction\namplitudes involving $\\pi$ absorption/production.",
"arxiv_id": "nucl-th/9312016",
"authors": [
"L. Canton",
"G. Cattapan"
],
"categories": [
"nucl-th"
],
"doi": "10.1103/PhysRevC.50.2761",
"journal_ref": "Phys.Rev.C50:2761-2767,1994",
"title": "Theory of Coupled Pion--Trinucleon Systems",
"url": "https://arxiv.org/abs/nucl-th/9312016"
},
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