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${{\mathit D}_{{{3}}}^{*}{(2750)}}$ WIDTH

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M203W

VALUE (MeV) EVTS DOCUMENT ID TECN CHG  COMMENT $\bf{ 66 \pm5}$ OUR AVERAGE $66$ $\pm10$ $\pm14$ 79k 1 AAIJ 2020 D LHCB ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$ $95.3$ $\pm9.6$ $\pm34.0$ 28k 2 AAIJ 2016 AH LHCB ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$ $105$ $\pm18$ $\pm24$ 3 AAIJ 2015 Y LHCB ${{\mathit B}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $74.4$ $\pm3.4$ $\pm37.0$ 14k AAIJ 2013 CC LHCB 0 ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}{{\mathit X}}$ $74.4$ $\pm3.4$ $\pm19.1$ 56k AAIJ 2013 CC LHCB 0 ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit X}}$ $66.7$ $\pm6.6$ $\pm10.5$ 20k AAIJ 2013 CC LHCB + ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}{{\mathit X}}$ $71$ $\pm6$ $\pm11$ 23.5k 4 DEL-AMO-SANCH.. 2010 P BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}{{\mathit X}}$ $60.9$ $\pm5.1$ $\pm3.6$ 11.3k 4 DEL-AMO-SANCH.. 2010 P BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit X}}$ • • We do not use the following data for averages, fits, limits, etc. • • $154$ $\pm27$ $\pm16$ 5 AAIJ 2015 Y LHCB ${{\mathit B}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ 1  From a full four-body amplitude analysis of the ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$ decay. 2  From the amplitude analysis in the model describing the ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ wave together with virtual contributions from the ${{\mathit D}^{*}{(2007)}^{0}}$ and ${{\mathit B}^{*0}}$ states, and components corresponding to the ${{\mathit D}_{{{2}}}^{*}{(2460)}^{0}}$, ${{\mathit D}_{{{1}}}^{*}{(2680)}^{0}}$, ${{\mathit D}_{{{3}}}^{*}{(2760)}^{0}}$, and ${{\mathit D}_{{{2}}}^{*}{(3000)}^{0}}$ resonances. 3  Modeling the ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{\mathit S}{\mathrm -wave}$ with the Isobar formalism. 4  The states observed in the ${{\mathit D}^{*}}{{\mathit \pi}}$ and ${{\mathit D}}{{\mathit \pi}}$ final states are not necessarily the same. 5  Modeling the ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{\mathit S}{\mathrm -wave}$ with the K-matrix formalism.

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