  By using a combined amplitude analysis of the $\gamma\gamma\rightarrow
D\bar{D}$ and $\gamma\gamma\rightarrow J/\psi\omega$ data, we demonstrate that
the $X(3915)$, which is quoted as a $J^{PC}=0^{++}$ state in the Particle Data
Group table, is favored by the data to be a $J^{PC}=2^{++}$ state appearing in
both channels, which means that the $X(3915)$ and the $X(3930)$ can be regarded
as the same $J^{PC}=2^{++}$ state. Meanwhile, the data also prefer a large
helicity-0 contribution of this tensor resonance to the amplitudes instead of
the helicity-2 dominance assumed by {\it BABAR}, which may indicate a sizable
portion of non-$q\bar q$ components in this state. Identifying the $X(3915)$
with the $X(3930)$ and abandoning the helicity-2 dominance for this tensor
state are helpful for the further understandings of the properties of this
state and also of the mysterious "$XYZ$" charmoniumlike resonances.
