\begin{document}$J^P={1}/{2}^-$\end{document}, \begin{document}${3}/{2}^-$\end{document}. We introduce an explicit P-wave between the two light quarks in the interpolating currents (these light quarks are antisymmetric in the flavor space, thus giving rise to the designation of Λ-type baryon) to investigate the \begin{document}$\Lambda_b$\end{document} and \begin{document}$\Xi_b$\end{document} states within the framework of the full QCD sum rules. The predicted masses show that \begin{document}$\Xi_b(6087)$\end{document} and \begin{document}$\Xi_b(6095/6100)$\end{document} could be the P-wave bottom-strange baryon states with spin-parity \begin{document}$J^P={1}/{2}^-$\end{document} and \begin{document}${3}/{2}^-$\end{document}, respectively; meanwhile, \begin{document}$\Lambda_b(5912)$\end{document} and \begin{document}$\Lambda_b(5920)$\end{document} could be the P-wave bottom baryon states with spin-parity \begin{document}$J^P={1}/{2}^-$\end{document} and \begin{document}${3}/{2}^-$\end{document}, respectively. Moreover, \begin{document}$\Lambda_b(5920)$\end{document} and \begin{document}$\Xi_b(6095/6100)$\end{document} may have two remarkable under-structures or Fock components at least."> The Λ-type <i>P</i>-wave bottom baryon states via the QCD sum rules -
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