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We study the ρB*B̅N* system solving the Faddeev equations in the fixed center approximation. The B*B̅N* system will be considered forming a cluster, and using the two-body ρB* unitarized scattering amplitudes in the local Hidden Gauge approach we find a new I(JPC) = 1(3−−) state. The mass of the new state corresponds to a two particle invariant mass of the ρB* system close to the resonant energy of the B*2(5747), indicating that the role of this J = 2 resonance is important in the dynamical generation of the new state

A three body state with J=3 in theρB*B̅N*interaction

A three body state with J=3 in theρB^**B̅N^interaction