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.
Analysis of the hidden-charm pentaquark candidates in the $J/\psi \Xi$ mass spectrum via the QCD sum rules
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abstract
In this work, we construct the color $\bar{\mathbf{3}}\bar{\mathbf{3}}\bar{\mathbf{3}}$ type local five-quark currents with the light quarks $qss$ in the flavor octet, and study the $qssc\bar{c}$ pentaquark states via the QCD sum rules in a comprehensive way, and we emphasize that we achieve two light-flavor octets. We obtain the mass spectrum of the hidden-charm-doubly-strange pentaquark states with the isospin-spin-parity $IJ^{P}=\frac{1}{2}{\frac{1}{2}}^-$, $\frac{1}{2}{\frac{3}{2}}^-$ and $\frac{1}{2}{\frac{5}{2}}^-$, which can be confronted to the experimental data in the future, especially in the process $\Xi_b^- \to P_{css}^-\phi \to J/\psi \Xi^- \phi $. As a byproduct, we observe that the lowest hidden-charm pentaquark states are not of the scalar-diquark-scalar-diquark-antiquark type, it is not suitable to refer to the scalar and axialvector diquarks as the "good" and "bad" diquarks, respectively.
fields
hep-ph 2years
2026 2verdicts
UNVERDICTED 2representative citing papers
Machine learning models trained on known hadron data and an extended Gürsey-Radicati mass formula predict masses for triply heavy baryons and numerous pentaquark states, agreeing with available data and forecasting unobserved states.
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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Comprehensive Mass Predictions: From Triply Heavy Baryons to Pentaquarks
Machine learning models trained on known hadron data and an extended Gürsey-Radicati mass formula predict masses for triply heavy baryons and numerous pentaquark states, agreeing with available data and forecasting unobserved states.