Abstract

We study boron, carbon, nitrogen, and oxygen isotopes with a newly constructed shell-model Hamiltonian developed from a monopole-based universal interaction (${V}_{MU}$). The present Hamiltonian can reproduce well the ground-state energies, energy levels, electric quadrupole properties, and spin properties of these nuclei in full $psd$ model space including $(0\ensuremath{-}3)\ensuremath{\hbar}\ensuremath{\omega}$ excitations. Especially, it correctly describes the drip lines of carbon and oxygen isotopes and the spins of the ground states of ${}^{10}$B and ${}^{18}$N while some former interactions such as WBP and WBT fail. We point out that the inclusion of $2\ensuremath{\hbar}\ensuremath{\omega}$ excitations is important in reproducing some of these properties. In the present $(0+2)\ensuremath{\hbar}\ensuremath{\omega}$ calculations small but constant $E2$ effective charges appear to work quite well. As the inclusion of the $2\ensuremath{\hbar}\ensuremath{\omega}$ model space makes a rather minor change, this seems to be related to the smallness of the ${}^{4}$He core. Similarly, the spin $g$ factors are very close to free values. The applicability of tensor and spin-orbit forces in free space, which are taken in the present Hamiltonian, is examined in shell-model calculations.

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