  In this work, we investigate the interactions between the charmed-strange
meson ($D_s, D_s^{*}$) in $H$-doublet and the (anti-)charmed-strange meson
($D_{s1}, D_{s2}^{*}$) in $T$-doublet, where the one boson exchange model is
adopted by considering the $S$-$D$ wave mixing and the coupled-channel effects.
By extracting the effective potentials for the discussed $H_s\bar{T}_s$ and
$H_s{T}_s$ systems, we try to find the bound state solutions for the
corresponding systems. We predict the possible hidden-charm hadronic molecular
states with hidden strangeness, i.e., the $D_s^{*}\bar D_{s1}+c.c.$ states with
$J^{PC}$=$0^{--}, 0^{-+}$ and the $D_s^{*}\bar D_{s2}^{*}+c.c.$ states with
$J^{PC}$=$1^{--}, 1^{-+}$. Applying the same theoretical framework, we also
discuss the $H_s T_s$ systems. Unfortunately, the existence of the open-charm
and open-strange molecular states corresponding to the $H_s T_s$ systems can be
excluded.
