$g$ factor of chiral doublets with $\pi {\left(1h_{11/2}\right)}^1\otimes \nu {\left(1h_{11/2}\right)}^{-1}$ configuration

The $g$ factor of chiral doublet bands has been extensively studied within the framework of the particle rotor model. Specifically, these investigations have focused on systems characterized by the particle-hole configuration $\pi {\left(1h_{11/2}\right)}^1\otimes \nu {\left(1h_{11/2}\right)}^{-1}$. Comprehensive examinations have been carried out to assess the influence of deformation parameters $\beta$ and $\gamma$, the moment of inertia $J_0$, the total spin $I$, and the angular momentum of the collective rotor $j_R$ on the $g$ factor. The findings reveal that the $g$ factor exhibits insensitivity to variations in $J_0$ and $\beta$ values, while its behavior is highly sensitive to changes in the $\gamma$ parameter. Moreover, it has been observed that the $g$ factors and the $g\left(j_R\right)$ plots associated with the doublet bands demonstrate remarkable similarity in the static chirality region. However, noticeable differences arise in regions characterized by chiral vibration or lacking chirality.