  Recently, the Belle collaboration measured the ratios of the branching
fractions of the newly observed $\Omega(2012)$ excited state. They did not
observe significant signals for the $\Omega(2012) \to \bar{K} \Xi^*(1530) \to
\bar{K} \pi \Xi$ decay, and reported an upper limit for the ratio of the three
body decay to the two body decay mode of $\Omega(2012) \to \bar{K} \Xi$. In
this work, we revisit the newly observed $\Omega(2012)$ from the molecular
perspective where this resonance appears to be a dynamically generated state
with spin-parity $3/2^-$ from the coupled channels interactions of the $\bar{K}
\Xi^*(1530)$ and $\eta \Omega$ in $s$-wave and $\bar{K} \Xi$ in $d$-wave. With
the model parameters for the $d$-wave interaction, we show that the ratio of
these decay fractions reported recently by the Belle collaboration can be
easily accommodated.
