  In this work, we propose the $4S$-$3D$ mixing scheme to assign the
$\Upsilon(10753)$ into the conventional bottomonium family. Under this
interpretation, we further study its hidden-bottom hadronic decays with a
$\eta^{(\prime)}$ or $\omega$ emission, which include
$\Upsilon(10753)\to\Upsilon(1S)\eta^{(\prime)}$, $\Upsilon(10753)\to
h_{b}(1P)\eta$ and $\Upsilon(10753)\to\chi_{bJ}\omega$ ($J$=0,1,2) processes.
Since the $\Upsilon(10753)$ is above the $B\bar{B}$ threshold, the
coupled-channel effect cannot be ignored, thus, when calculating partial decay
widths of these $\Upsilon(10753)$ hidden-bottom decays, we apply the hadronic
loop mechanism. Our result shows that these discussed decay processes own
considerable branching fractions with the order of magnitude of $10^{-4}\sim
10^{-3}$, which can be accessible at Belle II and other future experiments.
