Analysis of the hidden-charm pentaquark candidates in the J/ψΞ mass spectrum via the QCD sum rules

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 $Ξ_b^- \to P_{css}^-ϕ\to J/ψΞ^- ϕ$. 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.

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Publication Details

Journal
Nuclear Physics B
Published
2026-04-12
DOI
https://doi.org/10.1016/j.nuclphysb.2026.117456
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
0.00

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article

Analysis of the hidden-charm pentaquark candidates in the J/ψΞ mass spectrum via the QCD sum rules

Zhi-Gang Wang, Yang Liu
Nuclear Physics B
Quantum Chromodynamics and Particle Interactions
article

Analysis of the hidden-charm pentaquark candidates in the J/ψΞ mass spectrum via the QCD sum rules

Zhi-Gang Wang, Yang Liu
article en

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 $Ξ_b^- \to P_{css}^-ϕ\to J/ψΞ^- ϕ$. 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.

Nuclear Physics BVol. 1027
National Natural Science Foundation of China
Openalex Percentile: Top 97%
Quantum Chromodynamics and Particle Interactions
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