Abstract

The LHCb Collaboration has recently reported the observation for the first time of a spin-33 resonance in the heavy quark sector. They have shown that the Dˉ0K−\bar{D}^{0}K^{-} structure seen in the Bs0→Dˉ0K−π+B_{s}^{0}\to \bar{D}^{0}K^{-}π^{+} reaction and with invariant mass 2.86 GeV2.86\,{\rm GeV} is an admixture of a spin-11 and a spin-33 resonances. Motivated by the good agreement between our theoretical predictions some time ago and the properties extracted from the experiment of the Ds1∗(2860)D_{s1}^{\ast}(2860) and Ds3∗(2860)D_{s3}^{\ast}(2860) states, we perform an extension of the study of the strong decay properties of the DsJ∗(2860)D_{sJ}^{\ast}(2860) and present the same analysis for the Ds1∗(2700)D_{s1}^{\ast}(2700) and DsJ(3040)D_{sJ}(3040) mesons. This provides a unified and simultaneous description of the three higher excited charmed-strange resonances observed until now. For completeness, we present theoretical results for masses and strong decays of the low-lying charmed-strange mesons and those experimental missing states which belong to the spin-multiplets of the discovered Ds1∗(2700)D_{s1}^{\ast}(2700), DsJ∗(2860)D_{sJ}^{\ast}(2860) and DsJ(3040)D_{sJ}(3040) resonances. The theoretical framework used is a constituent quark model which successfully describes hadron phenomenology from light to heavy quark sectors.

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