  Currently, there is much controversy surrounding the interpretation of the
$\Xi(2030)$ and $\Xi(2012)$ as traditional hadrons containing double strange
quarks. In particular, the ratios of the partial decay widths into
$\Lambda\bar{K}$ and $\Sigma\bar{K}$ for $\Xi(2030)$ cannot obtain a suitable
explanation under the $qss$ three quark structure~\cite{Xiao:2013xi}. Thus, we
suggest the $\Xi(2030)$ and $\Xi(2012)$ to be
$VB(=\bar{K}^{*}\Sigma/\rho\Xi/\bar{K}^{*}\Lambda/\phi\Xi/\omega\Xi)$ molecular
states. In this work, we perform a systematical investigation of possible
molecular states from the
$VB(=\bar{K}^{*}\Sigma/\rho\Xi/\bar{K}^{*}\Lambda/\phi\Xi/\omega\Xi)$
interaction. The interaction of the system considered is described by the
$t$-channel vector ($\rho,\omega,\phi,\bar{K}^{*}$) and pseudoscalar
($\pi,\eta,\bar{K}$) mesons exchanges. By solving the non-relativistic
Schr\"{o}dinger equation with the obtained one-boson-exchange potentials, the
$VB(=\bar{K}^{*}\Sigma/\rho\Xi/\bar{K}^{*}\Lambda/\phi\Xi/\omega\Xi)$ bound
states with different quantum numbers are searched. The calculation suggests
that $\Xi(2030)$ can be assigned as a $P$-wave
$\bar{K}^{*}\Sigma/\rho\Xi/\bar{K}^{*}\Lambda/\phi\Xi/\omega\Xi$ molecular
state with spin parity $J^P=5/2^{+}$. The calculation also predict the
existence of four
$\bar{K}^{*}\Sigma/\rho\Xi/\bar{K}^{*}\Lambda/\phi\Xi/\omega\Xi$ bound states
with $J^P=1/2^{\pm}$ and $J^P=3/2^{\pm}$. The $\Xi(2012)$ may be a candidate
for one of these four bound states. If $\Xi(2012)$ is an $S$-wave molecular
state with $J^P=1/2^{-}$ or $J^P=3/2^{-}$, we suggest determining its spin and
parity by studying its decay width, owing to the difference in their molecular
components.
