The ${{\mathit \chi}_{{{c0}}}{(3915)}}$ was originally seen by BELLE in its ${{\mathit \omega}}{{\mathit J / \psi}}$ decay mode and was produced in both ${{\mathit B}}$ decays in CHOI 2005 and ${{\mathit \gamma}}{{\mathit \gamma}}$ collisions in UEHARA 2010. The $\mathit J{}^{PC}$ was determined to be ${}^{}0{}^{++}$ by BABAR in LEES 2012AD but this assignment was questioned by ZHOU 2015C. In AAIJ 2020AI LHCb found the ${{\mathit D}^{+}}{{\mathit D}^{-}}$ decay mode of the ${{\mathit \chi}_{{{c0}}}{(3915)}}$ using ${{\mathit B}}$ decays and determined its $\mathit J{}^{PC}$ to be ${}^{}0{}^{++}$. Based on their compatible mass, width, and $\mathit J{}^{PC}$, we assume the state decaying to ${{\mathit \omega}}{{\mathit J / \psi}}$ and the state decaying to ${{\mathit D}^{+}}{{\mathit D}^{-}}$ are both the ${{\mathit \chi}_{{{c0}}}{(3915)}}$. See also the ${{\mathit \chi}_{{{c2}}}{(3930)}}$.