$\Omega_c \eta$   $\Xi D^*$   $\Xi_c \bar{K}^*$   $\Xi^{\prime}_c\bar{K}^*$
  ----------------------- ---------------- ------------------------- -------------------- ----------------- ----------- ------------------- ---------------------------
           $g_i$           $-0.06+i0.14$       $\bf 1.94+i0.01$         $-2.14+i0.26$       $1.98+i0.01$         0               0                       0
      $g_i\,G^{II}_i$      $-1.40-i3.85$      $\bf -34.41-i0.30$         $9.33-i1.10$      $-16.81-i0.11$        0               0                       0
   ${\bf 3091.28+i5.12}$   $\Xi_c\bar{K}$   $\Xi^{\prime}_c\bar{K}$        $\Xi D$         $\Omega_c \eta$   $\Xi D^*$   $\Xi_c \bar{K}^*$   $\Xi^{\prime}_c\bar{K}^*$
           $g_i$            $0.18-i0.37$         $0.31+i0.25$          $\bf 5.83-i0.20$     $0.38+i0.23$         0               0                       0
      $g_i\,G^{II}_i$      $5.05+i10.19$         $-9.97-i3.67$        $\bf -29.82+i0.31$    $-3.59-i2.23$        0               0                       0

  : The coupling constants to various channels for the poles in the $J^P={1/2}^-$ sector, with $q_{max}=650$ MeV, and $g_i\,G^{II}_i$ in MeV.

\[res1\]

Next we look for the states of $J^P={3/2}^-$ from the pseudoscalar-baryon$({3/2}^+)$ interaction. In Table \[tabDij2\] we see that the pseudoscalar-baryon$({3/2}^+)$ states do not couple to vector-baryon and we can separate two blocks, the channels $\Xi^*_c\,\bar{K}$, $\Omega_c^*\,\eta$, $\Xi^*\,D$ and $\Xi\,D^*$, $\Xi_c\,\bar{K}^*$, $\Xi^{\prime}_c\,\bar{K}^*$. The first three channels in $s$-wave give rise to $J^P={3/2}^-$, while the other three give rise to $J^P={1/2}^-, {3/2}^-$, degenerated in our approach. We then separate these two sets of states.

In Table \[res3\] we show the results for $J^P={3/2}^-$ for different values of the cutoff. We see that we get two poles. Yet, if we choose the same cutoff as in the $J^P={1/2}^-$ sector we find a mass of $3125$ MeV and 