  We report on recent $BABAR$ analyses of the baryonic $B$ decays
$\bar{B}^{0}\to\Lambda_{\rm c}^{+}\bar{p}\pi^{+}\pi^{-}$, $B^{-}\to\Sigma_{\rm
c}^{++}\bar{p}\pi^{-}\pi^{-}$, $\bar{B}^{0}\to\Lambda_{\rm
c}^{+}\bar{p}p\bar{p}$ and $\bar{B}^{0}\to D^{0}\Lambda\bar{\Lambda}$. The used
data sample contains $471\times10^{6}\,B\bar{B}$ pairs that were generated in
the process $e^{+}e^{-}\to\Upsilon(4S)\to B\bar{B}$ and collected with the
$BABAR$ detector at the PEP-II storage ring at SLAC. We find ${\cal
B}(\bar{B}^{0}\to\Lambda_{\rm c}^{+}\bar{p}\pi^{+}\pi^{-}) = (12.3\pm0.5_{\rm
stat}\pm0.7_{\rm syst}\pm3.2_{\rm\Lambda_{\rm c}})\times10^{-3}$, ${\cal
B}(B^{-}\to\Sigma_{\rm c}^{++}\bar{p}\pi^{-}\pi^{-}) = (2.98\pm0.16_{\rm
stat}\pm0.15_{\rm syst}\pm0.77_{\rm\Lambda_{\rm c}})\times10^{-3}$, where the
last uncertainty is due to ${\cal B}(\Lambda_{\rm c}^{+}\to p K^{-}\pi^{+})$,
respectively. For the decay $\bar{B}^{0}\to\Lambda_{\rm c}^{+}\bar{p}p\bar{p}$
we see no events and set an upper limit ${\cal B}(\bar{B}^{0}\to\Lambda_{\rm
c}^{+}\bar{p}p\bar{p})\times \frac{{\cal B}(\Lambda_{\rm c}^{+}\to p
K^{-}\pi^{+})}{0.050} < 2.8\times10^{-6}$ at $90\,\%$ CL, where we have
normalized ${\cal B}(\Lambda_{\rm c}^{+}\to p K^{-}\pi^{+})$ to the world
average value. There is evidence for the decay $\bar{B}^{0}\to
D^{0}\Lambda\bar{\Lambda}$ and we measure ${\cal B}(\bar{B}^{0}\to
D^{0}\Lambda\bar{\Lambda}) = (9.8^{+2.9}_{-2.6}\,_{\rm stat}\pm1.9_{\rm
syst})\times10^{-6}$ corresponding to a significance of $3.4\sigma$.
