It has long been recognized that the P-to-s converted phases from the core-mantle boundary such as SKS, PKS, and SKKS (hereafter referred to as XKS) split into orthogonally polarized fast and slow components in azimuthally anisotropic media (Ando et al., 1983;Long & Silver, 2009;Savage, 1999;Silver & Chan, 1991). The two splitting parameters, the polarization orientation of the fast component (fast orientation or ϕ) and the time separation (splitting time or δt) between the two waves, reveal the orientation and splitting magnitude of the anisotropy, respectively. Over the past several decades, the shear wave splitting (SWS) analysis technique has been widely used to delineate azimuthal anisotropy in the upper mantle, where lattice preferred orientation of crystallographic axes of main constitute minerals such as olivine is the dominant cause of the observed anisotropy (Katayama &