Extends baryo-charmonium picture to c cbar ssq pentaquarks, predicting two negative-parity triplets with lowest kaon-associated state near 4.60 GeV and a near-degenerate doublet for upper kaon states.
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3 Pith papers cite this work. Polarity classification is still indexing.
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Pith papers citing it
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hep-ph 3years
2026 3verdicts
UNVERDICTED 3representative citing papers
The u-channel Lambda_c exchange enhances rescattering via Dbar(*) Sigma_c states in the piN to J/psiN reaction, producing clear peaks for Pc(4312) (1/2^-) and Pc(4457) (3/2^-) at microbarn cross sections while suppressing other states.
Hidden-charm pentaquarks do not appear in J/ψ photoproduction because rescattering from ar{D}^{(*)}Σ_c intermediate states is suppressed relative to ar{D}^{(*)}Λ_c by a factor of roughly five in the relevant couplings.
citing papers explorer
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Doubly-strange hidden-charm pentaquarks from the Fermi statistics of the light-quark cloud
Extends baryo-charmonium picture to c cbar ssq pentaquarks, predicting two negative-parity triplets with lowest kaon-associated state near 4.60 GeV and a near-degenerate doublet for upper kaon states.
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Probing hidden-charm pentaquarks from the $\pi N\rightarrow J/\psi N$ reaction
The u-channel Lambda_c exchange enhances rescattering via Dbar(*) Sigma_c states in the piN to J/psiN reaction, producing clear peaks for Pc(4312) (1/2^-) and Pc(4457) (3/2^-) at microbarn cross sections while suppressing other states.
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Nonexistence of hidden-charm pentaquarks in $J/\psi$ photoproduction
Hidden-charm pentaquarks do not appear in J/ψ photoproduction because rescattering from ar{D}^{(*)}Σ_c intermediate states is suppressed relative to ar{D}^{(*)}Λ_c by a factor of roughly five in the relevant couplings.