  We study color allowed bottom baryon to $s$-wave and $p$-wave charmed baryon
non-leptonic decays in this work. The charmed baryons include spin-1/2 and
spin-3/2 states. Explicitly, we consider $\Lambda_b\to \Lambda^{(*,**)}_c M^-$,
$\Xi_b\to\Xi_c^{(**)} M^-$ and $\Omega_b\to\Omega^{(*,**)}_c M^-$ decays with
$M=\pi, K, \rho, K^*, a_1, D, D_s, D^*, D^*_s$, $\Lambda^{(*,**)}_c=\Lambda_c,
\Lambda_c(2595), \Lambda_c(2625), \Lambda_c(2765), \Lambda_c(2940)$,
$\Xi_c^{(**)}=\Xi_c, \Xi_c(2815), \Xi_c(2790)$ and $\Omega^{(*,**)}_c=\Omega_c,
\Omega_c(2770), \Omega_c(3050), \Omega_c(3090), \Omega_c(3120)$. There are six
types of transitions, namely, (i) ${\cal B}_b({\bf \bar 3_f},1/2^+)$ to ${\cal
B}_c({\bf \bar 3_f},1/2^+)$, (ii) ${\cal B}_b({\bf 6_f},1/2^+)$ to ${\cal
B}_c({\bf 6_f},1/2^+)$, (iii) ${\cal B}_b({\bf 6_f},1/2^+)$ to ${\cal B}_c({\bf
6_f},3/2^+)$, (iv) ${\cal B}_b({\bf 6_f},1/2^+)$ to ${\cal B}_c({\bf
6_f},3/2^-)$, (v) ${\cal B}_b({\bf \bar 3_f},1/2^+)$ to ${\cal B}_c({\bf \bar
3_f},1/2^-)$, and (vi) ${\cal B}_b( {\bf \bar 3_f},1/2^+)$ to ${\cal B}_c({\bf
\bar 3_f},3/2^-)$ transitions. Types (i) to (iii) involve spin 1/2 and 3/2
$s$-wave charmed baryons, while types (iv) to (vi) involve spin 1/2 and 3/2
$p$-wave charmed baryons. The transition form factors are calculated in the
light-front quark model approach. All of the form factors in the $1/2\to 1/2$
and $1/2 \to 3/2$ transitions are extracted, and they are found to reasonably
satisfy the relations obtained in the heavy quark limit, as we are using heavy
but finite $m_b$ and $m_c$. Using na\"{i}ve factorization, decay rates and
up-down asymmetries of the above modes are predicted and can be checked
experimentally. The study on these decay modes may shed light on the quantum
numbers of $\Lambda_c(2765)$, $\Lambda_c(2940)$ $\Omega_c(3050)$,
$\Omega_c(3090)$ and $\Omega_c(3120)$.
