Isospin Symmetry Violation in the Strong Decays of the Spin-2 Exotic State X2(4014)

The isospin violation in the strong decays of the spin-2 exotic charmonium-like state $${{X}_{2}}(4014)$$ has been studied within the framework of the covariant confined quark model. We have interpreted the exotic hadron $${{X}_{2}}$$ as a four-quark state with a $$(D{\\text{*}}\\bar {D}*)$$ molecular-type interpolating quark current and computed the leading-order strong decay widths at the level of two-petal quark-loop diagrams. The partial widths of the decay modes into channels $${{\\omega \\,\\,J} \\mathord{\\left/ {\\vphantom {{\\omega \\,\\,J} \\Psi }} \\right. \\kern-0em} \\Psi }$$ and $${{\\rho }^{0}}{J \\mathord{\\left/ {\\vphantom {J \\Psi }} \\right. \\kern-0em} \\Psi }$$ , and their branching ratio recently discussed in literature have been calculated and analyzed. In the comparison of our approach to the recent $$(D{\\text{*}}\\bar {D}*)$$ molecular scenarios, we have shown the explicit appearance of the threshold effect in the latter models. The calculated partial strong decay widths and their branching ratio are in reasonable agreement with the latest experimental data.

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Publication Details

Journal
Physics of Particles and Nuclei
Published
2026-09-15
DOI
https://doi.org/10.1134/s1063779626701145
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
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Isospin Symmetry Violation in the Strong Decays of the Spin-2 Exotic State X2(4014)

Gurjav Ganbold
Physics of Particles and Nuclei
Quantum Chromodynamics and Particle Interactions
article

Isospin Symmetry Violation in the Strong Decays of the Spin-2 Exotic State X2(4014)

Gurjav Ganbold
article en

Abstract

The isospin violation in the strong decays of the spin-2 exotic charmonium-like state $${{X}_{2}}(4014)$$ has been studied within the framework of the covariant confined quark model. We have interpreted the exotic hadron $${{X}_{2}}$$ as a four-quark state with a $$(D{\text{*}}\bar {D}*)$$ molecular-type interpolating quark current and computed the leading-order strong decay widths at the level of two-petal quark-loop diagrams. The partial widths of the decay modes into channels $${{\omega \,\,J} \mathord{\left/ {\vphantom {{\omega \,\,J} \Psi }} \right. \kern-0em} \Psi }$$ and $${{\rho }^{0}}{J \mathord{\left/ {\vphantom {J \Psi }} \right. \kern-0em} \Psi }$$ , and their branching ratio recently discussed in literature have been calculated and analyzed. In the comparison of our approach to the recent $$(D{\text{*}}\bar {D}*)$$ molecular scenarios, we have shown the explicit appearance of the threshold effect in the latter models. The calculated partial strong decay widths and their branching ratio are in reasonable agreement with the latest experimental data.

Physics of Particles and NucleiVol. 57(5)
Mongolian Academy of Sciences (MN), Joint Institute for Nuclear Research (RU), Institute of Physics and Technology (MN)
Openalex Percentile: Top 12%
Quantum Chromodynamics and Particle Interactions
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