Exotic hadrons as heavy hadronic molecules and their partners

In 2022, the doubly charmed tetraquark $T_{cc}\sim cc\bar{u}\bar{d}$ was reported by LHCb. Since the exotic state is located just below the $DD^\ast$ threshold, it is considered to be a $DD^\ast$ molecule. In this talk, we study the $D^{(\ast)}D^{(\ast)}$ coupled channel systems in the meson exchange potential model. By tuning the cutoff parameter, the model explains $T_{cc}$ as a $D^{(\ast)}D^{(\ast)}$ molecule with $I(J^P)=0(1^+)$. Furthermore, by replacing $D$ with $\Xi_{cc}$ respecting the superflavor symmetry, new pentaquark $\bar{D}^{(\ast)}\Xi_{cc}^{(\ast)}$ is also investigated. We find a bound state for $I(J^P)=0(1/2^-)$ below the $\bar{D}\Xi_{cc}$ threshold. To form these bound states, the $\sigma$ exchange potential plays a dominant role to produce an attraction. In addition, the coupled-channel effect induced by the $\pi$ and $\rho$ exchange potentials support to generate an attraction.

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Publication Details

Published
2025-12-23
DOI
https://doi.org/10.22323/1.500.0074
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
0.00

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article

Exotic hadrons as heavy hadronic molecules and their partners

Yasuhiro Yamaguchi, Masayasu Harada, Tatsuya Asanuma
Quantum Chromodynamics and Particle Interactions
article

Exotic hadrons as heavy hadronic molecules and their partners

Yasuhiro Yamaguchi, Masayasu Harada, Tatsuya Asanuma
article en

Abstract

In 2022, the doubly charmed tetraquark $T_{cc}\sim cc\bar{u}\bar{d}$ was reported by LHCb. Since the exotic state is located just below the $DD^\ast$ threshold, it is considered to be a $DD^\ast$ molecule. In this talk, we study the $D^{(\ast)}D^{(\ast)}$ coupled channel systems in the meson exchange potential model. By tuning the cutoff parameter, the model explains $T_{cc}$ as a $D^{(\ast)}D^{(\ast)}$ molecule with $I(J^P)=0(1^+)$. Furthermore, by replacing $D$ with $\Xi_{cc}$ respecting the superflavor symmetry, new pentaquark $\bar{D}^{(\ast)}\Xi_{cc}^{(\ast)}$ is also investigated. We find a bound state for $I(J^P)=0(1/2^-)$ below the $\bar{D}\Xi_{cc}$ threshold. To form these bound states, the $\sigma$ exchange potential plays a dominant role to produce an attraction. In addition, the coupled-channel effect induced by the $\pi$ and $\rho$ exchange potentials support to generate an attraction.

Japan Society for the Promotion of Science
Openalex Percentile: Top 22%
Quantum Chromodynamics and Particle Interactions
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