  The challenges with the molecular model of the multiquark systems are the
identification of the hadronic molecules and the interaction between two color
neutral hadrons. We study the di-hadronic molecular systems with proposed
interaction potential as s-wave one boson exchange potential along with Screen
Yukawa-like potential, and arrived with the proposal that within hadronic
molecule the two color neutral hadrons experience the dipole-like interaction.
The present study is the continuation of our previous study
\cite{arxiv-Rathaud-penta}. With the proposed interaction potential, the mass
spectra of $\Sigma_{s}K^{*}$, $\Sigma_{c}K^{*}$, $\Sigma_{b}K^{*}$,
$\Sigma_{s}D^{*}$, $\Sigma_{c}D^{*}$, $\Sigma_{b}D^{*}$, $\Sigma_{s}B^{*}$,
$\Sigma_{c}B^{*}$, $\Sigma_{b}B^{*}$, $\Xi_{s}K^{*}$, $\Xi_{c}K^{*}$,
$\Xi_{b}K^{*}$, $\Xi_{s}D^{*}$, $\Xi_{c}D^{*}$, $\Xi_{b}D^{*}$, $\Xi_{s}B^{*}$,
$\Xi_{c}B^{*}$, $\Xi_{b}B^{*}$ meson-baryon molecules are predicted. The
Weinberg compositeness theorem which provides clue for the compositeness of the
state is used for determination of the scattering length and effective range.
The present study predict $P_{c}(4450)$ pentaquark sate as $\Sigma_{c}D^{*}$
molecule with $I(J^{P})=\frac{1}{2}(\frac{3}{2}^{-})$. The formalism also
predicts some very interesting open as well as hidden flavour near threshold
molecular pentaquark states.
