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${{\mathit D}_{{{0}}}^{*}{(2300)}^{\pm}}$ WIDTH

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M179W

VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT $\bf{ 221 \pm18}$ OUR AVERAGE $255$ $\pm26$ $\pm51$ 1 AAIJ 2015 X LHCB ${{\mathit B}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{+}}{{\mathit \pi}^{-}}$ $217$ $\pm13$ $\pm13$ 2 AAIJ 2015 Y LHCB ${{\mathit B}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ • • We do not use the following data for averages, fits, limits, etc. • • $230$ $\pm15$ $\pm21$ 3 AAIJ 2015 Y LHCB ${{\mathit B}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $283$ $\pm24$ $\pm34$ 18.8k 4 LINK 2004 A FOCS ${{\mathit \gamma}}$ A 1  From the Dalitz plot analysis including various ${{\mathit K}^{*}}$ and ${{\mathit D}^{**}}$ mesons as well as broad structures in the ${{\mathit K}}{{\mathit \pi}}{\mathit S}{\mathrm -wave}$ and the ${{\mathit D}}{{\mathit \pi}}$ $\mathit S$- and ${\mathit P}{\mathrm -wave}$s. 2  Modeling the ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{\mathit S}{\mathrm -wave}$ with the Isobar formalism. 3  Modeling the ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{\mathit S}{\mathrm -wave}$ with the K-matrix formalism. 4  Possibly the feed-down from another state.

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