  In the diquark-diantiquark composition, we study the masses of hidden charm
tetraquark systems ($cq\bar{c}\bar{q}$, $cs\bar{c}\bar{s}$ and
$cs\bar{c}\bar{q}$) using a linear confinement potential. In this study, we
have factorized the four body system into three subsequent two body systems. To
remove degeneracy in the S and P wave masses of mesons and tetraquark states,
the spin-spin, spin orbit and tensor components of the confined one gluon
exchange interactions are employed. In this attempt, we have been able to
assign the $\psi(4230)$ as pure $cq\bar{c}\bar{q}$ tetraquark state.
$\psi(4360)$ and $\psi(4390)$ as pure $cs\bar{c}\bar{q}$ tetraquark states.
According to our analysis $\psi(4260)$ is an admixture of $^1P_1$ and $^5P_1$
$cq\bar{c}\bar{q}$ tetraquark state. Additionally, we have been able to predict
the radiative decay width $\Gamma_{(\psi \rightarrow J/\psi \gamma)}$, leptonic
decay width $\Gamma_{e^+e^-}$ and hadronic decays of $1^{--}$ tetraquark stat
