  Recently, scientists have made great progresses in experiments in searching
for the excited states of $\Xi_{b}$ and $\Lambda_{b}$ baryons such as the
$\Lambda_{b}(6072)$, $\Lambda_{b}(6146)$, $\Lambda_{b}(6152)$, $\Xi_{b}(6227)$,
$\Xi_{b}(6100)$, $\Xi_{b}(6327)$ and $\Xi_{b}(6333)$. Stimulated by these
progresses, we give a systematical analysis about the $1D$ and $2D$ states of
$\Xi_{b}$ and $\Lambda_{b}$ baryons with the method of QCD sum rules. By
constructing three types of interpolating currents, we calculate the masses and
pole residues of these heavy baryons with different excitation modes
$(L_{\rho},L_{\lambda})=(0,2)$, $(2,0)$ and $(1,1)$. As a result, we decode the
inner structures of $\Lambda_{b}(6146)$, $\Lambda_{b}(6152)$, $\Xi_{b}(6327)$
and $\Xi_{b}(6333)$, and favor assigning these states as the $1D$ baryons with
the quantum numbers $(L_{\rho},L_{\lambda})=(0,2)$ and $\frac{3}{2}^{+}$,
$\frac{5}{2}^{+}$, $\frac{3}{2}^{+}$ and $\frac{5}{2}^{+}$, respectively. In
addition, the predictions about the masses and pole residues of the other $1D$
and $2D$ states of $\Xi_{b}$ and $\Lambda_{b}$ baryons in this paper are
helpful in studying the D-wave bottom baryons in experiments in the future.
