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Stimulated by the measurement of the $J\psi\phi$ decay model of $Y(4274)$ bythe LHCb Collaboration, we consider a possible interpretation of this state asa hadron molecular-a bound state of $D_s$ and $\bar{D}_{s0}(2317)$ mesons.Using effective Lagrangian approach, we calculate the two-body strong decaychannels $Y(4274)\to{}J/\psi\phi,\chi_{c0}\eta,\chi_{c0}\eta,D^{*}_s\bar{D}_s$,$D\bar{D}^{*}$, $K\bar{K}^{*}$, and $\phi\phi$ through hadronic loops andthree-body decays into $\pi^0{}D_s\bar{D}_s$. In comparison with the LHCb data,our results show that $Y(4274)$ cannot be assigned to be a$D_s\bar{D}_{s0}(2317)$ molecular state. The calculated partial decay widthswith $J^P=1^{+}$ $D_s\bar{D}_{s0}$ molecular state picture indicates thatallowed decay modes, $\chi_{c0}\eta$ and $\chi_{c1}\eta$, may have the smallestbranching ratio and are of the order of 0.0 MeV. Future experimentalmeasurements of such two processes can be quite useful to test the differentinterpretations of the $Y(4274)$. If $P-$wave $D_s\bar{D}_{s0}$ molecular exist[we marked as $Y^{'}(4274)$], the total decay is at the order of 1.06-1.84 MeV,which seems to be within the reach of the current experiments such as Belle II.In addition, the calculated partial decay widths indicate that allowed decaymode, $D\bar{D}^{*}$, may have the biggest branching ratio. The experimentalmeasurements for this strong decay process could be a crucial to observe such anew state $Y^{'}(4274)$.

Possible $P$- wave $D_s\bar{D}_{s0}(2317)$ molecular state $Y^{'}(4274)$