  To better understand the nature and internal structure of the exotic states
discovered by many collaborations, more information on their electromagnetic
properties and their strong and weak interactions with other hadrons is needed.
The residue or current coupling constant of these states together with their
mass are the main inputs in determinations of such properties. We perform QCD
sum rules analyses on the hidden-charm pentaquark states with spin-parities $
J^{P}= \frac{3}{2}^{\pm}$ and $ J^{P}= \frac{5}{2}^{\pm}$ to calculate their
residue and mass. In the calculations, we adopt a molecular picture for $
J^{P}= \frac{3}{2}^{\pm}$ states and a mixed current in a molecular form for $
J^{P}= \frac{5}{2}^{\pm}$. Our analyses show that the $P_c^+(4380)$ and
$P_c^+(4450)$, observed by LHCb Collaboration, can be considered as
hidden-charm pentaquark states with $ J^{P}= \frac{3}{2}^{-}$ and $ J^{P}=
\frac{5}{2}^{+}$, respectively.
