Impurity effects of the Λ hyperon in the hypernuclear systems ${}_{{\rm{\Lambda }}}^{25}\mathrm{Mg}$ and ${}_{{\rm{\Lambda }}}^{29}\mathrm{Si}$
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Impurity effects of the Λ hyperon in the hypernuclear systems ${}_{{\rm{\Lambda }}}^{25}\mathrm{Mg}$ and ${}_{{\rm{\Lambda }}}^{29}\mathrm{Si}$ |
| Ji-Wei Cui,Xian-Rong Zhou |
| Figure 1. Potential energy surfaces as functions of deformation parameter β, derived from mean-field calculation, for 24Mg and ${}_{\,{\rm{\Lambda }}}^{25}$ Mg (panel (a)), and for 28Si and ${}_{\,{\rm{\Lambda }}}^{29}$ Si (panel (b)). ${\rm{\Lambda }}1$, ${\rm{\Lambda }}2$, ${\rm{\Lambda }}3$ and ${\rm{\Lambda }}4$ represent different hyperonic orbitals and correspond to ${\rm{\Lambda }}[000]1/{2}^{+}$, ${\rm{\Lambda }}[110]1/{2}^{-}$, ${\rm{\Lambda }}[101]3/{2}^{-}$ and Λ[101]1/2−, respectively. |
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