The Particle Data Group has assigned the X(3915) meson, an ωJ/ψ mass peak seen in B → KωJ/ψ decays and γγ → ωJ/ψ two-photon fusion reactions, as the χc0(2P ), the 2 3 P0 charmonium state. Here it is shown that if the X(3915) is the χc0(2P ), the measured strength of the γγ → X(3915) signal implies an upper limit on the branching fraction B(χc0(2P ) → ωJ/ψ) < 7.8% that conflicts with a > 14.3% lower limit derived for the same quantity from the B → KX(3915) decay rate. Also, the absence any signal fordecays is used to establish the limit B(X(3915) → D 0D0 < 1.2 × B(X(3915) → ωJ/ψ). This contradicts expectations that χc0(2P ) decays to D 0D0 would be a dominant process, while decays to ωJ/ψ, which are Okubo-Zweig-Iizuka suppressed, would be relatively rare. These, plus reasons given earlier by Guo and Meissner, raise serious doubts about the X(3915) = χc0(2P ) assignment.