  We studied the radiative transitions between the $\Upsilon(10753)$, the
$S$-$D$ mixed state of the $\Upsilon(4S)$ and $\Upsilon_1(3\,{}^3D_1)$, and the
$X_b$, the heavy quark flavor symmetry counterpart of the $X(3782)$ in the
bottomonium sector. The radiative transition was assumed to occur through the
intermediate bottom mesons, including $P$-wave $B_1^{(\prime)}$ mesons as well
as the $S$-wave $B^{(*)}$ ones. The consideration of the $B_1^{(\prime)}$
mesons leads to the couplings to be in $S$-wave, and hence enhances the
contributions of the intermediate meson loops. The radiative decay width for
the $\Upsilon(10753)\to\gamma X_b$ is predicted to be order of
$10~\mathrm{keV}$, corresponding to a branching fraction of $10^{-4}$. Based on
the theoretical results, we strongly suggest to search for the $X_b$ in the
$e^+e^-\to\gamma X_b$ with $X_b\to\pi\pi\chi_{b1}$ near
$\sqrt{s}=10.754~\mathrm{GeV}$, and it is hoped that the calculations here
could be tested by the future Belle II experiments.
