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Updated analysis of charmonium states in a relativized quark potential model

Published 20 Apr 2025 in hep-ph and hep-ex | (2504.14575v1)

Abstract: Motivated by recent experimental observations of charmonium(-like) states, we investigate their interpretation as conventional charmonium states within the framework of relativized quark potential model. We find a consistent description of the updated masses of charmonia, bottomonia and some selected charmed mesons, then systematically compute open-charm strong decay widths and electromagnetic transition widths for radially excited charmonium states up to n=5n=5. The numerical results show significantly improved agreement with experimental masses and widths. Notably, the newly-observed χc1(4010)\chi_{c1}(4010) and χc1(4274)\chi_{c1}(4274) are tentatively associated with the χc1(2P)\chi_{c1}(2P) and χc1(3P)\chi_{c1}(3P) respectively, while the χc0(4500)\chi_{c0}(4500) and χc0(4700)\chi_{c0}(4700) are interpreted as the χc0(4P)\chi_{c0}(4P) and χc0(5P)\chi_{c0}(5P) states. For the controversial χc1(3872)\chi_{c1}(3872) state, we suggest its potential connection to χc1(4010)\chi_{c1}(4010), as a two-pole structure due to the χc1(2P)\chi_{c1}(2P) coupling to DDˉD\bar{D} channels. Intriguingly, the predicted mass of χc0(2P)\chi_{c0}(2P) is about 3851 MeV, diverging from the original estimate of 3916 MeV in the Godfrey and Isgur's work but consistent with non-relativistic potential model predictions. This calculation might provide more insight to the future experimental investigation of charmonium(-like) states.

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