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.
Where is the next pentaquark state?
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
The LHCb Collaboration has observed two types of hidden-charm pentaquark states $P_{\psi}^N$ and $P_{\psi s}^{\Lambda}$ since 2015. In this work, we predict two other types of hidden-charm pentaquark states $P_{\psi s}^{\Sigma}(4367)$ and $P_{\psi ss}^{N}(4379)$ within the framework of heavy pentaquark chiral perturbation theory. We suggest the LHCb Collaboration to observe $P_{\psi ss}^{N}(4379)^{-}$ and $P_{\psi ss}^{N}(4379)^0$ with $J^P=\frac{1}{2}^{-}$ in the $J/\psi \Xi$ spectrum through amplitude analyses of $\Omega_b^- \to J/\psi \Xi^0 K^-$ decays and $B^- \to J/\psi \Xi^- \bar{\Lambda}$ decays.
citation-role summary
citation-polarity summary
fields
hep-ph 1years
2025 1verdicts
CONDITIONAL 1roles
background 1polarities
unclear 1representative citing papers
citing papers explorer
-
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.