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From the perspective that the $\Lambda_c(2595)$ and $\Lambda_c(2625)$ aredynamically generated resonances from the $DN,~D^*N$ interaction and coupledchannels, we have evaluated the rates for $\Lambda_b \to \pi^- \Lambda_c(2595)$and $\Lambda_b \to \pi^- \Lambda_c(2625)$ up to a global unknown factor thatallows us to calculate the ratio of rates and compare with experiment, wheregood agreement is found. Similarly, we can also make predictions for the ratioof rates of the, yet unknown, decays of $\Lambda_b \to D_s^- \Lambda_c(2595)$and $\Lambda_b \to D_s^- \Lambda_c(2625)$ and make estimates for theirindividual branching fractions.

$\Lambda_b \to \pi^- (D_s^-) \Lambda_c(2595),~\pi^- (D_s^-) \Lambda_c(2625)$ decays and $DN,~D^*N$ molecular components