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Our recently proposed model of the $\Delta(1600)$ resonance, in which thedominant component is a quasi-bound state of the $\Delta(1232)$ and the pion,is confronted with a similar model of the $N^*(1440)$ resonance as itscounterpart in the P11 partial wave. We stress an essentially differentmechanism responsible for generating the two resonances.

The enigmatic $\Delta(1600)$ resonance