Abstract

In nuclear physics, triton and helium-3 nucleus can be understood as three-body hadronic molecules. Analogous to the loosely bound structures for the triton and helium-3 nucleus, whether there is a bound state formed by three hadrons leaves us an open issue. Based on the one-boson exchange model as well as the adoption of the variational approach, we make a comprehensive investigation on the tritonlike systems of three identical baryons N N N , Λ Λ Λ , Ξ Ξ Ξ , and Σ Σ Σ . We predict that the three-body molecular states for the systems of three identical hadrons of baryon octet are probably existent as long as their two-body subsystems have bound states. The numerical results of this work may be helpful for the theoretical and experimental researches on the trihadron molecules in future.

Highlights

  • Numerous exotic states called “XYZ” reported in the last few decades pose great challenges to the traditional quark model [1,2,3,4,5,6,7,8,9,10,11]

  • One may believe that it describe the dynamics of triton well

  • We have constructed the formalism of the BOP method for a general system consists of the three identical fermions with half spin

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Summary

Introduction

Numerous exotic states called “XYZ” reported in the last few decades pose great challenges to the traditional quark model [1,2,3,4,5,6,7,8,9,10,11]. The scenario of dihadron molecule was first motivated by the deuteron, in which a proton and a neutron form a loosely bound state by colorless strong interactions. The existence of triton leaves us an interesting question that whether an identical three-body system composed of the other members in the octet of the 1/2+ baryon has a bound state. In the present work we shall perform investigations on the three-body systems composed of the identical hadrons from the octet of the 1/2+ baryon.

Formalism
CCCA: ð6Þ
CCCCCCCCA
Ni N1j
CCCCCCCCCCA ij ca
Applications to the Baryon Octet
Summary
The Matrix Element of the H aaH aa
The Isospin Wave Functions of the Relevant Systems

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