Likely existence of bound states and the Efimov effect in the triple-$J/\psi$ system

TL;DR

This paper predicts the existence of bound states and the Efimov effect in the triple-$J/\psi$ system, providing theoretical support for future experimental searches of fully-charmed hexaquark states.

Contribution

It introduces a theoretical study of the triple-$J/\psi$ system using the Gaussian expansion method, revealing potential bound states and Efimov effect, which are novel insights in this context.

Findings

Supports the existence of a triple-$J/\psi$ bound state.

Suggests the presence of the Efimov effect in the system.

Extends analysis to triple-$\Upsilon(1S)$ system with similar results.

Abstract

The ground-breaking discovery of the first fully charmed tetraquark state $X(6900)$ in the $J/\psi J/\psi$ invariant mass distribution by the LHCb collaboration has inspired intensive theoretical studies. Various interpretations, such as molecular states, compact tetraquark states, and coupled-channel effects, have been proposed for these states. Of particular interest is the ongoing search for the triple-$J/\psi$ state--a fully-charmed hexaquark state. To deepen our understanding of the triple-$J/\psi$ state and to guide future experimental searches, we study the triple-$J/\psi$ system in this work employing the Gaussian expansion method and the $J/\psi J/\psi$ potential parameterized to yield a shallow bound state, as suggested in several theoretical works. Our results support a triple-$J/\psi$ bound state, even in cases where the attractive interaction between the two $J/\psi$ mesons is very weak. Moreover, our analysis implies the Efimov effect in the triple-$J/\psi$ system. In addition, we extend our investigation to the triple-$\Upsilon (1S)$ system and obtain results similar to those for the triple-$J/\psi$ system.