  We use the method of QCD sum rules within the framework of heavy quark
effective theory to study the mass spectrum of the $\Sigma_{b}(6097)^{\pm}$ and
$\Xi_{b}(6227)^{-}$, and use the method of light-cone sum rules still within
the heavy quark effective theory to study their decay properties. Our results
suggest that they can be well interpreted as $P$-wave bottom baryons with the
spin-parity $J^P = 3/2^-$. They belong to the baryon doublet $[\mathbf{6}_F, 2,
1, \lambda]$, where the total and spin angular momenta of the light degree of
freedom are $j_l = 2$ and $s_l = 1$, and the orbital angular momentum is
between the bottom quark and the two-light-quark system ($\lambda$-type). This
doublet contains six bottom baryons, and we predict masses (mass differences)
and decay widths of the other four states to be $M_{\Omega_b(3/2^-)} = 6.46 \pm
0.12 {~\rm GeV}$, $\Gamma_{\Omega_b(3/2^-)} = 58{^{+65}_{-33}} {~\rm MeV}$,
$M_{\Sigma_b(5/2^-)}-M_{\Sigma_b(3/2^-)}= 13 \pm 5 {~\rm MeV}$,
$M_{\Xi_b^{\prime}(5/2^-)}-M_{\Xi_b^{\prime}(3/2^-)} = 12 \pm 5 {~\rm MeV}$,
and $M_{\Omega_b(5/2^-)}-M_{\Omega_b(3/2^-)} = 11 \pm 5 {~\rm MeV}$. We propose
to search for them in further LHCb experiments.
