Examination of the φ-NN bound-state problem with lattice QCD $ N-φ $ potentials

The developed Faddeev three-body equations are solved to search for bound-state solutions of a phi-meson (φ) and two nucleons ( NN ) system. The newly published spin $ 3/2 $ N-φ potential based on the (2+1)-flavor lattice QCD simulations near physical point, and realistic NN Malfliet-Tjon (MT) potential, are employed. Our numerical calculations for (I)Jπ=(0)2⁻ φ-d system in maximum spin leads to ground state binding energy of about $ 7 $ MeV and a matter radius of about $ 8 $ fm. Our results indicates the possibility of the formation of new nuclear clusters.