In the diquark-antidiquark composition, we study the masses of hidden charm tetraquark systems ($cq\overline{c}\overline{q}$, $cs\overline{c}\overline{s}$ and $cs\overline{c}\overline{q}$) 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 $cq\overline{c}\overline{q}$ tetraquark state. $\psi (4360)$ and $\psi (4390)$ as pure $cs\overline{c}\overline{q}$ tetraquark states. According to our analysis $\psi (4260)$ is found to be an admixture of two ${}^{1}P_1$ $cq\overline{c}\overline{q}$ tetraquark states having mass 4259 MeV. Additionally, we have been able to predict the radiative decay width ${\mathrm{\Gamma }}_{(\psi \to J/\psi \gamma )}$, leptonic decay width ${\mathrm{\Gamma }}_{e^{+}{e}^{-}}$ and hadronic decays of $1^{--}$ tetraquark states. The status of X(3872) and $Z_{c}s$ are also identified as compact tetraquark states. Additionally, we have been able to predict the radiative decay width ${\mathrm{\Gamma }}_{(\psi \to J/\psi \gamma )}$, leptonic decay width ${\mathrm{\Gamma }}_{e^{+}{e}^{-}}$ and hadronic decays of $1^{--}$ tetraquark states.

在双夸克-反双夸克的构成中，我们研究了隐藏的魅力四夸克系统的质量（$Cq\overline{C}\overline{q}$， $Cs\overline{C}\overline{s}$ 和 $Cs\overline{C}\overline{q}$）使用线性限制电位。在这项研究中，我们将四个身体系统分解为三个随后的两个身体系统。为了消除介子和四夸克态在S波和P波质量中的简并性，采用了有限的一种胶子交换相互作用的自旋自旋，自旋轨道和张量分量。在此尝试中，我们已经能够分配$\psi （4230）$ 如纯 $Cq\overline{C}\overline{q}$ 四夸克状态。 $\psi （4360）$ 和 $\psi （4390）$ 如纯 $Cs\overline{C}\overline{q}$四夸克状态。根据我们的分析$\psi （4260）$ 被发现是两种的混合物 ${}^{\mathrm{1个}}P_{\mathrm{1个}}$ $Cq\overline{C}\overline{q}$具有质量4259 MeV的四夸克态。此外，我们已经能够预测辐射衰减宽度${\mathrm{\Gamma }}_{（\psi \to Ĵ/\psi \gamma ）}$，轻子衰变宽度 ${\mathrm{\Gamma }}_{{Ë}^{+}{Ë}^{-}}$ 和强子衰变 ${\mathrm{1个}}^{--}$四夸克状态。X（3872）和的状态${ž}_{C}s$也被确定为紧密四夸克态。此外，我们已经能够预测辐射衰减宽度${\mathrm{\Gamma }}_{（\psi \to Ĵ/\psi \gamma ）}$，轻子衰变宽度 ${\mathrm{\Gamma }}_{{Ë}^{+}{Ë}^{-}}$ 和强子衰变 ${\mathrm{1个}}^{--}$ 四夸克状态。