Abstract With the advancement of first-principles calculations for baryon–baryon interactions, it becomes possible to obtain reliable hyperon–nucleon potentials by lattice QCD simulations with the HAL QCD method. High-precision few-body methods, such as the Gaussian Expansion Method (GEM), are applicable to solve quantum few-body systems up to four- and five-body systems. By combining the HAL QCD potentials with the GEM, one can predict the level structure of novel hypernuclei prior to experimental observation. In this review, we utilize the lattice QCD N N Ξ potential obtained by the HAL QCD method to investigate the few-body systems NN N N Ξ and NNN N N N Ξ. Our analysis indicates that the lightest bound Ξ hypernucleus is the NNN N N N Ξ system. To extract detailed information on the isospin and spin components of the N N Ξ interaction, we perform a four-body calculation for the N α α N Ξ system with the total isospin T = 0 T = 0 and T = 1 T = 1. We demonstrate that the level structure of this system is sensitive to the isospin and spin dependencies of the N N Ξ interaction. Furthermore, we propose experimental investigations to produce the NNN N N N Ξ and N α α N Ξ systems via the (K^-, K^+) (K -, K +) and (K^-, K⁰) (K -, K 0)
Hiyama et al. (2025) studied this question.