Tri-meson state
arXiv:2411.03589 · doi:10.1103/PhysRevD.111.034002
Abstract
We systematically explore the trimeson states with various isospin-spin configurations in the quark model by solving exactly the six-body Schrödinger equations with the Gaussian expansion method. The configuration is not only approximately 10.2 MeV lower than the threshold of its constituent particles but also about 0.2 MeV below that of the compact tetraquark state and . This configuration manifests a loose two-body bound state composed of and , with a size of around 4.75 fm. In contrast, the configurations , , and exhibit binding energies of less than 1 MeV relative to their constituent particles, establishing a loose three-meson bound state. After coupling three configurations with , the trimeson state with remains a loosely two-body bound state with a binding energy around 1.5 MeV and a huge size of 2.20 fm, in which the configuration is dominant, contributing to the overall probability. Among the four bound configurations, the -meson exchange plays a decisive role. The meson pair , resembling the short-range strong correlated - pair in nuclear physics, prevails over other types of meson pairs. The meson pair not only contributes to the binding mechanisms but also influences the spatial structures of those stable trimeson configurations.
10 pages, 3 figures, 3 tables
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