A simple analytic expression of the three-body wave function describing the system $(\alpha\alpha n)$ in the ground state $\frac{ 3}{ 2}^-$ of ${ }^9\mathrm{ Be}$ is obtained. In doing this, it is assumed that the $\alpha$ particles interact with each other via the $S$-wave Ali-Bodmer potential including the Coulomb term, and the neutron-$\alpha$ 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 $\alpha\alpha$ 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 Schr\"odinger equation for experimentally known binding energy and for the $\alpha\alpha$ potential whose difference from the Ali-Bodmer one is minimized by varying the adjustable parameters which the postulated wave function depends on.
Categories: nucl-th