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Is the $$N Omega$$ dibaryon system bound in a meson exchange model?

Sekihara, Takayasu; Kamiya, Yuki*; Hyodo, Tetsuo*

Recently, the HAL QCD simulation pointed out that the $$N Omega$$ interaction is strongly attractive enough to generate a bound state with spin/parity $$J^{P} = 2^{+}$$. In this talk, we investigate the origin of the attraction of the $$N Omega$$ interaction by constructing a meson exchange model. Between $$N$$ and $$Omega$$, $$eta$$ and scalar-isoscalar ("$$sigma$$") mesons can be exchanged. The couplings between the $$eta$$ meson and baryons are fixed by the effective Lagrangian based on flavor symmetry. For the "$$sigma$$" exchange, on the other hand, we employ the correlated two meson exchange developed in the study of the nuclear force. We discuss whether the $$N Omega$$ interaction is attractive or not and whether the attraction is strong enough to generate the $$N Omega$$ bound state or not.

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