\begin{document}$ B^- B^{*-} $\end{document}, \begin{document}$ B^0 B^{*-} $\end{document}, \begin{document}$ B^- B^{*0} $\end{document}, \begin{document}$ B^0 B^{*0} $\end{document}, \begin{document}$ B_s^0 B^{*-} $\end{document}, \begin{document}$ B^- B_s^{*0} $\end{document}, \begin{document}$ B_s^{0} B^{*0} $\end{document}, \begin{document}$ B^0 B_s^{*0} $\end{document}, and \begin{document}$ B^0_s B_s^{*0} $\end{document} states are extracted using light-cone sum rules. We explore the magnetic dipole moments of these states in a molecular picture with spin-parity \begin{document}$ J^P = 1^+ $\end{document}. The magnetic dipole moments of hadrons include useful information on the distributions of internal charge and magnetization, which can be used to understand their geometrical shapes and quark-gluon organization. The results of the present study along with the spectroscopic parameters may help future theoretical and experimental research on the characteristics of doubly-bottom tetraquark states."> Magnetic dipole moments of <inline-formula><tex-math id="M1">\begin{document}${{\boldsymbol{B_{(\boldsymbol s)}^{(\bf *)} B_{(\boldsymbol s)}^{(\bf *)}}}}$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/05c15b24-37a1-4ec7-99a8-1bc47f7554d0/CPC-2022-0328_M1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/05c15b24-37a1-4ec7-99a8-1bc47f7554d0/CPC-2022-0328_M1.png"/></alternatives></inline-formula> states -
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