Production of doubly charmed tetraquark T via photon-photon fusion at electron-positron colliders

Within a phenomenological diquark fragmentation model, we study the production of doubly charmed tetraquark T c c via photon-photon fusion at electron-positron colliders. The production of T c c is divided into two steps: the perturbative production of heavy ( c c ) -diquark and its nonperturbative hadronization. Two diquark configurations of ( c c ) [ S 1 3 ] 3 ¯ and ( c c ) [ S 0 1 ] 6 are considered, and the ( c c ) [ S 1 3 ] 3 ¯ state dominates the production of T c c . We discuss two hadronization models of ( c c ) [ S 1 3 ] 3 ¯ intermediate state into the tetraquark T c c . It is found that it is promising to observe the tetraquark T c c via photon-photon fusion process both at the Circular Electron Positron Collider (CEPC) and the International Linear Collider (ILC). We find that the cross sections are sensitive to constituent charm quark mass of diquark, and they also have strong dependence on the hadronization models.

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Publication Details

Journal
Physics Letters B
Published
2025-05-09
DOI
https://doi.org/10.1016/j.physletb.2025.139543
Citations
2
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
3.74

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article

Production of doubly charmed tetraquark T via photon-photon fusion at electron-positron colliders

Shi-Yuan Li, Yan-Rui Liu, Jun Jiang, Xiao Liang et al.
2 citations
Physics Letters B
Quantum Chromodynamics and Particle Interactions
3.74
article

Production of doubly charmed tetraquark T via photon-photon fusion at electron-positron colliders

Shi-Yuan Li, Yan-Rui Liu, Jun Jiang, Xiao Liang, Zong-Guo Si, Zhong-Juan Yang
article en
2 citations

Abstract

Within a phenomenological diquark fragmentation model, we study the production of doubly charmed tetraquark T c c via photon-photon fusion at electron-positron colliders. The production of T c c is divided into two steps: the perturbative production of heavy ( c c ) -diquark and its nonperturbative hadronization. Two diquark configurations of ( c c ) [ S 1 3 ] 3 ¯ and ( c c ) [ S 0 1 ] 6 are considered, and the ( c c ) [ S 1 3 ] 3 ¯ state dominates the production of T c c . We discuss two hadronization models of ( c c ) [ S 1 3 ] 3 ¯ intermediate state into the tetraquark T c c . It is found that it is promising to observe the tetraquark T c c via photon-photon fusion process both at the Circular Electron Positron Collider (CEPC) and the International Linear Collider (ILC). We find that the cross sections are sensitive to constituent charm quark mass of diquark, and they also have strong dependence on the hadronization models.

Physics Letters BVol. 866
Shandong University (CN), University of Jinan (CN)
National Natural Science Foundation of China, Natural Science Foundation of Shandong Province
Openalex Percentile: Top 8%
Quantum Chromodynamics and Particle Interactions
3.74
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Production of doubly charmed tetraquark T via photon-photon fusion at electron-positron colliders — Shi-Yuan Li, Yan-Rui Liu, et al. · Physics Letters B (2025) | TGRS Research Map | TGRS