  In this work, we investigate the $\Upsilon(10753)\to\Upsilon(1^3D_J)\eta$
($J=1,2,3$) processes, where the $\Upsilon(10753)$ is assigned as a
conventional bottomonium under the $4S$-$3D$ mixing scheme. Our result shows
that the concerned processes have considerable branching ratios, {\it i.e.},
branching ratios $\mathcal{B}[\Upsilon(10753)\to\Upsilon(1^3D_{1})\eta]$ and
$\mathcal{B}[\Upsilon(10753)\to\Upsilon(1^3D_{2})\eta]$ can reach up to the
order of magnitude of $10^{-4}-10^{-3}$, while
$\mathcal{B}[\Upsilon(10753)\to\Upsilon(1^3D_{3})\eta]$ is around
$10^{-6}-10^{-5}$. With the running of Belle II, it is a good opportunity for
finding out the concerned hidden-bottom hadronic decays.
