Search for hidden-charm tetraquark with strangeness in $e^{+}{e}^{-}\to K^{+}{D}_s^{\ast -}{D}^{\ast 0}+c.c.$

Abstract

We report a search for a heavier partner of the recently observed $Z_{cs}(3985{)}^{-}$ state, denoted as $Z_{cs}^{\prime -}$, in the process $e^{+}{e}^{-}\to K^{+}{D}_s^{\ast -}{D}^{\ast 0}+c.c.$, based on $e^{+}{e}^{-}$ collision data collected at the center-of-mass energies of $\sqrt{s}=4.661$, 4.682 and 4.699 GeV with the BESIII detector. The $Z_{cs}^{\prime -}$ is of interest as it is expected to be a candidate for a hidden-charm and open-strange tetraquark. A partial-reconstruction technique is used to isolate $K^{+}$ recoil-mass spectra, which are probed for a potential contribution from $Z_{cs}^{\prime -}\to D_s^{\ast -}{D}^{\ast 0}$ ($c.c.$). We find an excess of $Z_{cs}^{\prime -}\to D_s^{\ast -}{D}^{\ast 0}$ ($c.c.$) candidates with a significance of $2.1\sigma$, after considering systematic uncertainties, at a mass of $(4123.5\pm 0.7_{stat.}\pm 4.7_{syst.})\mathrm{MeV}/c^2$. As the data set is limited in size, the upper limits are evaluated at the 90\% confidence level on the product of the Born cross sections (${\sigma }^{\mathrm{Born}}$) and the branching fraction ($\mathcal{B}$) of $Z_{cs}^{\prime -}\to D_s^{\ast -}{D}^{\ast 0}$, under different assumptions of the $Z_{cs}^{\prime -}$ mass from 4.120 to 4.140 MeV and of the width from 10 to 50 MeV at the three center-of-mass energies. The upper limits of ${\sigma }^{\mathrm{Born}}\cdot \mathcal{B}$ are found to be at the level of $\mathcal{O}(1)$ pb at each energy. Larger data samples are needed to confirm the $Z_{cs}^{\prime -}$ state and clarify its nature in the coming years.

arXiv comment17 pages, 7 figures

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