We have studied the Gamow-Teller (GT) transitions from $N=Z+2$ neighbors to $N=Z=$ odd nuclei in $p$-shell region by using isospin-projected and $\beta\gamma$-constraint antisymmetrized molecular dynamics combined with generator coordinate method. The calculated GT transition strengths from $0^+1$ states to $1^+0$ states such as ${ }^{ 6} \textrm{ He}(0_1^+1)\rightarrow{ }^{ 6} \textrm{ Li}(1_1^+0)$, ${ }^{ 10} \textrm{ Be}(0_1^+1)\rightarrow{ }^{ 10} \textrm{ B}(1_1^+0)$, and ${ }^{ 14} \textrm{ C}(0_1^+1)\rightarrow{ }^{ 14} \textrm{ N}(1_2^+0)$ exhaust more than 50\% of the sum rule. These $N=Z+2$ initial states and $N=Z=$ odd final states are found to dominantly have $S=0,T=1$ $nn$ pairs and $S=1,T=0$ $pn$ pairs, respectively. Based on two-nucleon ($NN$) pair picture, we can understand the concentration of the GT strengths as the spin-isospin-flip transition $nn(S=0,T=1)\rightarrow pn(S=1,T=0)$ in $LS$-coupling scheme. The GT transition can be a good probe to identify the spin-isospin partner states with $nn$ pairs and $pn$ pairs of $N=Z+2$ and $N=Z=$ odd nuclei, respectively.
Categories: nucl-th