Hidden-Charm Strong Decays of Charmonium-Like State Y(4230)

We have studied hidden-charm strong decays of the charmonium-like resonant state $$Y(4320)$$ within the framework of a confined quark model by interpreting the resonance as a four-quark state with molecular-type interpolating current. The strong decay of $$Y$$ into a vector and a scalar resonance, with the latter decaying, subsequently to a pair of charged pseudoscalar states, has been investigated. We have calculated the partial widths of the strong decays $$Y \to {{\pi }^{ + }}{{\pi }^{ - }}{J \mathord{\left/ {\vphantom {J \Psi }} \right. \kern-0em} \Psi }$$ and $$Y \to {{K}^{ + }}{{K}^{ - }}{J \mathord{\left/ {\vphantom {J \Psi }} \right. \kern-0em} \Psi }$$ , and their branching ratio, which is recently determined by the BESIII Collaboration. The estimated proportion of branching and the calculated partial strong decay widths are in reasonable agreement with the most recent experimental results.

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Publication Details

Journal
Physics of Particles and Nuclei
Published
2024-08-01
DOI
https://doi.org/10.1134/s1063779624700175
Citations
1
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
0.66
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article

Hidden-Charm Strong Decays of Charmonium-Like State Y(4230)

Gurjav Ganbold
1 citations
Physics of Particles and Nuclei
Quantum Chromodynamics and Particle Interactions
0.66
article

Hidden-Charm Strong Decays of Charmonium-Like State Y(4230)

Gurjav Ganbold
article en
1 citations

Abstract

We have studied hidden-charm strong decays of the charmonium-like resonant state $$Y(4320)$$ within the framework of a confined quark model by interpreting the resonance as a four-quark state with molecular-type interpolating current. The strong decay of $$Y$$ into a vector and a scalar resonance, with the latter decaying, subsequently to a pair of charged pseudoscalar states, has been investigated. We have calculated the partial widths of the strong decays $$Y \to {{\pi }^{ + }}{{\pi }^{ - }}{J \mathord{\left/ {\vphantom {J \Psi }} \right. \kern-0em} \Psi }$$ and $$Y \to {{K}^{ + }}{{K}^{ - }}{J \mathord{\left/ {\vphantom {J \Psi }} \right. \kern-0em} \Psi }$$ , and their branching ratio, which is recently determined by the BESIII Collaboration. The estimated proportion of branching and the calculated partial strong decay widths are in reasonable agreement with the most recent experimental results.

Physics of Particles and NucleiVol. 55(4)
Mongolian Academy of Sciences (MN), Joint Institute for Nuclear Research (RU), Institute of Physics and Technology (MN)
Sustainable cities and communities, Climate action
Openalex Percentile: Top 15%
Quantum Chromodynamics and Particle Interactions
0.66
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