Amplitude Analysis of the Decays ηπ+ππ0 and ηπ0π0π0

dc.contributor.authorMitchell, R.E.
dc.date.accessioned2025-02-20T15:49:05Z
dc.date.available2025-02-20T15:49:05Z
dc.date.issued2017-01-10
dc.description.abstractBased on a sample of $1.31 \times 10^9$ $J/\psi$ events collected with the BESIII detector, an amplitude analysis of the isospin-violating decays $\eta^\prime \rightarrow \pi^+\pi^-\pi^0$ and $\eta^\prime \rightarrow \pi^0\pi^0\pi^0$ is performed. A significant $P$-wave contribution from $\eta^\prime \rightarrow \rho^{\pm} \pi^{\mp}$ is observed for the first time in $\eta^\prime \rightarrow \pi^+\pi^-\pi^0$. The branching fraction is determined to be ${\mathcal B}(\eta^\prime \rightarrow \rho^{\pm}\pi^{\mp})=(7.44\pm0.60\pm1.26\pm1.84)\times 10^{-4}$, where the first uncertainty is statistical, the second systematic, and the third model dependent. In addition to the nonresonant $S$-wave component, there is a significant $\sigma$ meson component. The branching fractions of the combined $S$-wave components are determined to be ${\mathcal B}(\eta^\prime \rightarrow \pi^+\pi^-\pi^0)_S=(37.63\pm0.77\pm2.22\pm4.48)\times 10^{-4}$ and ${\mathcal B}(\eta^\prime \rightarrow \pi^0\pi^0\pi^0)=(35.22\pm0.82\pm2.54)\times 10^{-4}$, respectively. The latter one is consistent with previous BESIII measurements.
dc.identifier.citation"Amplitude Analysis of the Decays $\eta^\prime \rightarrow \pi^+\pi^-\pi^0$ and $\eta^\prime \rightarrow \pi^0\pi^0\pi^0$." Physical Review Letters, vol. 118, no. 1, 2017-1-10, https://doi.org/10.1103/PhysRevLett.118.012001.
dc.identifier.issn1079-7114
dc.identifier.otherBRITE 983
dc.identifier.urihttps://hdl.handle.net/2022/30990
dc.language.isoen
dc.relation.isversionofhttps://doi.org/10.1103/PhysRevLett.118.012001
dc.relation.isversionofhttps://arxiv.org/abs/1606.03847v3
dc.relation.journalPhysical Review Letters
dc.rightsThis work may be protected by copyright unless otherwise stated.
dc.titleAmplitude Analysis of the Decays $\eta^\prime \rightarrow \pi^+\pi^-\pi^0$ and $\eta^\prime \rightarrow \pi^0\pi^0\pi^0$

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