\begin{document}$ B_{1}(5721) $\end{document}, \begin{document}$ B_{2}^{*}(5747) $\end{document}, \begin{document}$ B_{s1}(5830) $\end{document} and \begin{document}$ B_{s2}^{*}(5840) $\end{document} and identify possible assignments of \begin{document}$ B_{J}(5840) $\end{document} and \begin{document}$ B_{J}(5970) $\end{document}, we study the strong decay of these states with the \begin{document}$ ^{3}P_{0} $\end{document} decay model. Our analysis supports the assignments of \begin{document}$ B_{1}(5721) $\end{document} and \begin{document}$ B_{2}^{*}(5747) $\end{document} as the \begin{document}$ 1P_{1}' $\end{document} and \begin{document}$ 1^{3}P_{2} $\end{document} states, and \begin{document}$ B_{s1}(5830) $\end{document} and \begin{document}$ B_{s2}^{*}(5840) $\end{document} as the strange partners of \begin{document}$ B_{1}(5721) $\end{document} and \begin{document}$ B_{2}^{*}(5747) $\end{document}. Besides, we tentatively identify the recently observed \begin{document}$ B_{J}(5840) $\end{document} and \begin{document}$ B_{J}(5970) $\end{document} as the \begin{document}$ 2^{3}S_{1} $\end{document} and \begin{document}$ 1^{3}D_{3} $\end{document} states. It is noted that these conclusions need further confirmation by measurements of the decay channels \begin{document}$ B_{J}(5840)\rightarrow B\pi $\end{document} and \begin{document}$ B_{J}(5970)\rightarrow B\pi $\end{document} ."> Analysis of the excited bottom and bottom-strange states <i>B</i><sub>1</sub>(5721), <inline-formula><tex-math id="M2">\begin{document}${{ B_{2}^{*}(5747) }}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M2.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M2.png"/></alternatives></inline-formula>, <inline-formula><tex-math id="M3">\begin{document}${{ B_{s1}(5830)}} $\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M3.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M3.png"/></alternatives></inline-formula>, <inline-formula><tex-math id="M4">\begin{document}$ {{B_{s2}^{*}(5840) }}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M4.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M4.png"/></alternatives></inline-formula>, <inline-formula><tex-math id="M5">\begin{document}${{ B_{J}(5840) }}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M5.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M5.png"/></alternatives></inline-formula> and <inline-formula><tex-math id="M6">\begin{document}$ {{B_{J}(5970) }}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M6.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/4873f6a4-f7eb-4a8b-8464-1575f85c32ee/CPC-2019-0392_M6.png"/></alternatives></inline-formula> of the <i>B</i> meson family -
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