Strong decays of $T_{c\bar s0}(2900)^{++/0}$ as a fully open-flavor tetraquark state

TL;DR

This paper investigates the strong decay properties of the $T_{car s0}(2900)$ tetraquark candidate, calculating decay widths and branching ratios using QCD sum rules, and finds results consistent with experimental data.

Contribution

It provides a theoretical analysis of the decay modes and widths of the $T_{car s0}(2900)$ as a fully open-flavor tetraquark, offering predictions for experimental verification.

Findings

Full decay width estimated as 161.7±94.8 MeV.

Main decay channels are $D_s\pi$ and $DK$.

Predicted branching ratios guide future experimental searches.

Abstract

We have studied the strong decay properties of the recently observed $T^a_{c\bar s0}(2900)^{++/0}$ by considering it as a $cu\bar{d}\bar{s}/cd\bar{u}\bar{s}$ fully open-flavor tetraquark state with $I(J^P)=1(0^+)$. In the framework of QCD sum rules, we have calculated the three-point correlation functions of the two-body strong decay processes $T^a_{c\bar s0}(2900)^{++}\rightarrow D_s^+\pi^+$, $D^+K^+, D_s^{\ast +}\rho^+$ and $D_{s1}^+\pi^+$. The full width of $T^a_{c\bar s0}(2900)^{++/0}$ is obtained as $161.7\pm94.8$ MeV, which is consistent with the experimental observation. We predict the relative branching ratios as $\Gamma (T\rightarrow D_s\pi):\Gamma(T\rightarrow DK):\Gamma (T\rightarrow D_s^{\ast} \rho):\Gamma (T\rightarrow D_{s1}\pi)\approx1.00:1.10:0.04:0.43$, implying that the main decay modes of $T^a_{c\bar s0}(2900)^{++/0}$ state are $D_s\pi$ and $DK$ channels in our calculations. However, the $P$-wave decay mode $D_{s1}\pi$ is also comparable and important by including the uncertainties. To further identify the nature of $T^a_{c\bar s0}(2900)^{++/0}$, we suggest confirming them in the $DK$ and $D_{s}\pi$ final states, and measuring the above ratios in future experiments.