Abstract

In this work, we investigate the decays of the fully open-flavor tetraquark state ${X}_{0}(2900)$ which was observed by the LHCb collaboration very recently. By using an effective Lagrangian approach, the partial widths of ${X}_{0}(2900)$ are estimated, where ${X}_{0}(2900)$ is assumed to be an $S$-wave ${\overline{D}}^{*}{K}^{*}$ hadronic molecule with $I=0$. It is found that the estimated results are in agreement with the experimental observations. Moreover, we also predict the decay behaviors of the other unobserved ${\stackrel{\texttildelow{}}{X}}_{J(J=1,2)}$, which are the spin partners of the ${X}_{0}(2900)$ in the $S$-wave ${\overline{D}}^{*}{K}^{*}$ picture. It is pointed out that the ${\stackrel{\texttildelow{}}{X}}_{1}$ state with $I=0$ is a broad state with the width more than 100 MeV, while another ${\stackrel{\texttildelow{}}{X}}_{2}$ state with $I=0$ is a narrow state with the width approaching half of that for the ${X}_{0}(2900)$. In addition, our results also show that the ${\overline{D}}^{*}K$ mode is expected to be the dominant decay mode for both ${\stackrel{\texttildelow{}}{X}}_{1}$ and ${\stackrel{\texttildelow{}}{X}}_{2}$. Searching for those unobserved ${\stackrel{\texttildelow{}}{X}}_{J(J=1,2)}$ in the future experiments might be helpful to understand the nature of ${X}_{0}(2900)$.

Highlights

  • Until now, the exotic family is no longer thin due to the great efforts from the experimental side

  • In the hadronic molecule scenario, one may remind that the X0ð2900Þ was explained as a D ÃKÃ molecule [25,26,28,29,31,33,35,38,41], where it was naturally considered to be bounded via the S-wave interaction between the D Ã and KÃ and carried the quantum numbers JP 1⁄4 0þ since the angular momentum of the X0ð2900Þ is 0 from the LHCb measurements [16,17]

  • The obtained partial decay width for the X0 → D K process is in agreement with the experimental data with the model parameters Λ and Λ1 that are selected to be around 1 GeV

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Summary

INTRODUCTION

The exotic family is no longer thin due to the great efforts from the experimental side. The observed channel of X0ð2900Þ and X1ð2900Þ indicates that the quark components of these two states are cdsu Such kinds of exotic states have usually been considered as good candidates of tetraquark state, such as hadronic molecular states and compact tetraquark states. In the hadronic molecule scenario, one may remind that the X0ð2900Þ was explained as a D ÃKÃ molecule [25,26,28,29,31,33,35,38,41], where it was naturally considered to be bounded via the S-wave interaction between the D Ã and KÃ and carried the quantum numbers JP 1⁄4 0þ since the angular momentum of the X0ð2900Þ is 0 from the LHCb measurements [16,17].

EFFECTIVE LAGRANGIANS AND DECAYS
D Ã0μðx þ wKÃ
NUMERICAL RESULTS AND DISCUSSION
SUMMARY
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