  In this work we calculate the ratios of rates of the $\Xi_b$ nonleptonic and
semileptonic decays into the $\Xi_c$(2790) and $\Xi_c$(2815) ($\Xi_c^*$)
resonances. These resonances are dynamically generated from the
pseudoscalar-baryon and vector-baryon interactions, whose mixing is done using
the chiral Weinberg-Tomozawa (WT) meson-baryon interaction extended to four
flavors. The first part of the decay is a weak decay that we analyze through
their quark constituents where it is noted that only the heavy quarks ($b$ and
$c$) participate in the interaction, leaving the light pair ($ds$) as
spectators. This first decay then produces a meson-baryon pair that creates the
$\Xi_c^*$ through the WT interaction. We then proceed to calculate the decay
rates to $\Xi_c$(2790) and $\Xi_c$(2815) for both the nonleptonic and
semileptonic cases and then calculate the ratios between them. We do this
calculation nonrelativistically and fully relativistically and notice that,
even though both approaches yield somewhat different results in the rates, the
ratios are very similar (difference on the order of 1\%) in both cases. The
absolute values of the decay rates are also successfully calculated by
obtaining the rates between our decays and $\Lambda_b \to \pi (D_s ) \
\Lambda_c (2595) \left(\Lambda_c (2625) \right)$ and $\Lambda_b \to \bar{\nu}_l
l \ \Lambda_c (2595) \left(\Lambda_c (2625) \right)$ for which there are
experimental results, since the momentum transfer is similar such we can cancel
out the influence of the quark wave functions in the ratios.
