Using two LHCb pentaquark masses as inputs, this paper predicts the masses of the unseen P_Sigma_psi_s and P_Nss states from next-to-leading-order chiral perturbation theory.
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Masses of hidden-charm pentaquark states with $J^P = \frac{3}{2}^-$
Using two LHCb pentaquark masses as inputs, this paper predicts the masses of the unseen P_Sigma_psi_s and P_Nss states from next-to-leading-order chiral perturbation theory.