Wave function of $^9$Be in the three-body (alpha-alpha-n)-model

Fuente: arXiv
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Main Author: Rakityansky, S. A.
Format: Preprint
Published: 2024
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author Rakityansky, S. A.
author_facet Rakityansky, S. A.
contents A simple analytic expression of the three-body wave function describing the system $(ααn)$ in the ground state $\frac{3}{2}^-$ of ${}^9\mathrm{Be}$ is obtained. In doing this, it is assumed that the $α$ particles interact with each other via the $S$-wave Ali-Bodmer potential including the Coulomb term, and the neutron-$α$ forces act only in the $P$-wave state. This wave function is constructed by trial and error method via solving in this way a kind of inverse problem when the two-body $αα$ potential is recovered from a postulated three-body wave function. As a result, the wave function is an exact solution of the corresponding three-body Schrödinger equation for experimentally known binding energy and for the $αα$ potential whose difference from the Ali-Bodmer one is minimized by varying the adjustable parameters which the postulated wave function depends on.
format Preprint
id arxiv_https___arxiv_org_abs_2407_17371
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Wave function of $^9$Be in the three-body (alpha-alpha-n)-model
Rakityansky, S. A.
Nuclear Theory
A simple analytic expression of the three-body wave function describing the system $(ααn)$ in the ground state $\frac{3}{2}^-$ of ${}^9\mathrm{Be}$ is obtained. In doing this, it is assumed that the $α$ particles interact with each other via the $S$-wave Ali-Bodmer potential including the Coulomb term, and the neutron-$α$ forces act only in the $P$-wave state. This wave function is constructed by trial and error method via solving in this way a kind of inverse problem when the two-body $αα$ potential is recovered from a postulated three-body wave function. As a result, the wave function is an exact solution of the corresponding three-body Schrödinger equation for experimentally known binding energy and for the $αα$ potential whose difference from the Ali-Bodmer one is minimized by varying the adjustable parameters which the postulated wave function depends on.
title Wave function of $^9$Be in the three-body (alpha-alpha-n)-model
topic Nuclear Theory
url https://arxiv.org/abs/2407.17371