  We calculate the effective potentials of the $\Xi_c\bar{D}^{(\ast)}$,
$\Xi_c^\prime\bar{D}^{(\ast)}$ and $\Xi_c^\ast\bar{D}^{(\ast)}$ systems with
the chiral effective field theory up to the next-to-leading order. We
simultaneously consider the short-, intermediate- and long-range interactions.
With the newly observed $P_c$ spectra as inputs, we construct the quark-level
contact Lagrangians to relate the low energy constants to those of
$\Sigma_c\bar{D}^{(\ast)}$ with the help of quark model. Our calculation
indicates there are seven bound states in the $I=0$ strange hidden charm
$[\Xi_c^\prime\bar{D}^{(\ast)}]_J~(J=\frac{1}{2},\frac{3}{2})$ and
$[\Xi_c^\ast\bar{D}^{(\ast)}]_J~(J=\frac{1}{2},\frac{3}{2},\frac{5}{2})$
systems. Our analyses also disfavor the $\Lambda_c\bar{D}^{(\ast)}$ bound
states. However, we obtain three new hadronic molecules in the isoscalar
$[\Xi_c\bar{D}^{(\ast)}]_J~(J=\frac{1}{2},\frac{3}{2})$ systems. The masses of
$[\Xi_c\bar{D}]_{1/2}$, $[\Xi_c\bar{D}^{\ast}]_{1/2}$ and
$[\Xi_c\bar{D}^{\ast}]_{3/2}$ are predicted to be $4319.4^{+2.8}_{-3.0}$ MeV,
$4456.9^{+3.2}_{-3.3}$ MeV and $4463.0^{+2.8}_{-3.0}$ MeV, respectively. We
also notice the one-eta-exchange influence is rather feeble. Binding solutions
in the $I=1$ channels are nonexistent. We hope the future analyses at LHCb can
seek for these new $P_{cs}$s in the $J\psi\Lambda$ final states, especially
near the thresholds of $\Xi_c\bar{D}^{(\ast)}$.
