The pentaquark from a combined effective field theory and phenomenological perspective
arXiv:2011.01915 · doi:10.1140/epjc/s10052-021-09416-x
Abstract
The observation of the by the LHCb collaboration adds a new member to the set of known hidden-charm pentaquarks, which includes the , and . The is expected to have the light-quark content of a baryon (, ), but its spin is unknown. Its closeness to the threshold -- in the isospin-symmetric limit -- suggests the molecular hypothesis as a plausible explanation for the . While in the absence of coupled-channel dynamics heavy-quark spin symmetry predicts the two spin-states of the to be degenerate, power counting arguments indicate that the coupling with the nearby and channels might be a leading order effect. This generates a hyperfine splitting in which the pentaquark will be lighter than the configuration, which we estimate to be of the order of . We also point out an accidental symmetry between the and potentials. Finally, we argue that the spectroscopy and the decays of the might suggest a marginal preference for over .
16 pages, 1 figure; includes discussions on power counting, the J=1/2,3/2 hyperfine splitting, saturation, phenomenological relation between the Pcs(4459) and Pc(4440/4457) potentials, decay to , etc
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