[en] Recently, the Belle collaboration measured the ratios of the branching fractions of the newly observed Ω(2012) excited state. They did not observe significant signals for the Ω(2012)→$\stackrel{¯<!--\; ??\; -->}{K}$Ξ∗(1530)→$\stackrel{¯<!--\; ??\; -->}{K}$πΞ decay, and reported an upper limit for the ratio of the three body decay to the two body decay mode of Ω(2012)→$\stackrel{¯<!--\; ??\; -->}{K}$Ξ. In this work, we revisit the newly observed Ω(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 $\stackrel{¯<!--\; ??\; -->}{K}$Ξ∗(1530) and ηΩ in s-wave and $\stackrel{¯<!--\; ??\; -->}{K}$Ξ 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.