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${{\mathit D}_{{{s3}}}^{*}{(2860)}^{+}}$ MASS

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M226M

VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT $2860.5$ $\pm2.6$ $\pm6.5$ 1 AAIJ 2014 AW LHCB ${{\mathit B}_{{{s}}}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ • • We do not use the following data for averages, fits, limits, etc. • • $2867.1$ $\pm4.3$ $\pm1.9$ 3.1k AAIJ 2016 AW LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit K}_S^0}$ ${{\mathit X}}$ at 7, 8 TeV $2866.1$ $\pm1.0$ $\pm6.3$ 36k 2, 3 AAIJ 2012 AU LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ( ${{\mathit D}}{{\mathit K}}){}^{+}{{\mathit X}}$ at 7 TeV $2862$ $\pm2$ ${}^{+5}_{-2}$ 3122 4, 2 AUBERT 2009 AR BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{(*)}}{{\mathit K}}{{\mathit X}}$ $2856.6$ $\pm1.5$ $\pm5.0$ 5 AUBERT,BE 2006 E BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}}{{\mathit K}}{{\mathit X}}$ 1  Separated from the spin-1 component ${{\mathit D}_{{{s1}}}^{*}{(2860)}^{-}}$ by a fit of the helicity angle of the ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}$ system, with a statistical significance of the spin-3 and spin-1 components in excess of 10 $\sigma $. 2  Possible contribution from the ${{\mathit D}_{{{s1}}}^{*}{(2860)}}$ state. 3  From the combined fit of the ${{\mathit D}^{+}}{{\mathit K}_S^0}$ and ${{\mathit D}^{0}}{{\mathit K}^{+}}$ modes in the model including the ${{\mathit D}_{{{s2}}}^{*}{(2573)}^{+}}$, ${{\mathit D}_{{{s1}}}^{*}{(2700)}^{+}}$ and spin-0 ${{\mathit D}_{{{sJ}}}^{*}{(2860)}^{+}}$. 4  From simultaneous fits to the two ${{\mathit D}}{{\mathit K}}$ mass spectra and to the total ${{\mathit D}^{*}}{{\mathit K}}$ mass spectrum. 5  Superseded by AUBERT 2009AR.

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