$α+{}^2n+{}^2n$ 3-body cluster structures and dineutron breaking in ${}^8 \mathrm{He}$

Abstract

The $0_2^+$ state of ${}^8\mathrm{He}$ has been discovered by a recent experiment, which suggested a developed cluster structure of spatially correlated neutron pairs, called "dineutrons" (${}^2n$). We aim to investigate the structure of ${}^8\mathrm{He}(0^+_1)$ and ${}^8\mathrm{He}(0^+_2)$ to clarify the monopole excitation mode in ${}^8\mathrm{He}$ system while focusing on the $α+{}^2n+{}^2n$ cluster structures and the breaking of ${}^2n$ clusters. We apply a microscopic cluster model with the generator coordinate method for the $α+{}^2n+{}^2n$ cluster and ${}^6\mathrm{He}+{}^2n$ cluster dynamics. The $p_{3/2}$-closure component, which is induced by the spin-orbit force, is also incorporated. The present calculation reasonably reproduces the experimental data of the properties of ${}^8\mathrm{He}$, such as $2n$ and $4n$ separation energies, energy spectra, and radii. The spatially developed cluster structure of the $0_2^+$ state is obtained. The $0_1^+$ and $0_2^+$ states have dominant components of $α+{}^2n+{}^2n$ 3-body cluster, but contain significant ${}^2n$ breaking components which contribute to the energy gain and size shrinking of the ${}^8\mathrm{He}$ system. The monopole excitation in ${}^8\mathrm{He}$ is regarded as a radial excitation, which is similar to that in ${}^{12}\mathrm{C}$. The $α+{}^2n+{}^2n$ cluster structures play a dominant role in ${}^8\mathrm{He}(0_{1,2}^+)$, and the mixing of the dineutron breaking contributes to significant structural effects.