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In this work, we investigated the decays of the fully open-flavor tetraquarkstate $X_0(2900)$ which was observed by the LHCb Collaboration very recently.Here, the $X_0(2900)$ was assigned as a $S-$wave $\bar D^\ast K^\ast$ hadronicmolecule with $I=0$, and the effective lagrangian approach was applied toestimate the partial decay widths. Moreover, we also predicted the decaybehaviors of the other unobserved $X_{J(J=1,2)}$, which were the spin partnersof the $X_0(2900)$ in the $S-$wave $\bar D^\ast K^\ast$ picture. It was pointedout that the $X_1$ state with $I=0$ was a broad state with the width more thanone hundred MeV, while another $X_2$ state with $I=0$ was a narrow state withthe width approaching half of that for the $X_0(2900)$. In addition, ourresults also showed that the $\bar D^\ast K$ mode was expected to be thedominant decay mode for both $X_1$ and $X_2$. Searching for those unobserved$X_{J(J=1,2)}$ in the future experiments might be helpful to understand thenature of $X_0(2900)$.

A study of the decays of $S-$wave $\bar D^\ast K^\ast$ hadronic molecules: the scalar $X_0(2900)$ and its spin partners $X_{J(J=1,2)}$