Observation of the decay $h_{c}\to3(π^{+}π^{-})π^{0}$ (2403.03500v1)
Abstract: Based on $(2712.4\pm14.1)\times10{6}$ $\psi(3686)$ events collected with the BESIII detector, we study the decays $h_{c}\to3(\pi{+}\pi{-})\pi{0}$, $h_{c}\to2(\pi{+}\pi{-})\omega$, $h_{c}\to2(\pi{+}\pi{-})\pi{0}\eta$, $h_{c}\to2(\pi{+}\pi{-})\eta$, and $h_{c}\to p\bar{p}$ via $\psi(3686)\to\pi{0}h_{c}$. The decay channel $h_{c}\to3(\pi{+}\pi{-})\pi{0}$ is observed for the first time, and its branching fraction is determined to be $\left( {9.28\pm 1.14 \pm 0.77} \right) \times {10{ - 3}}$, where the first uncertainty is statistical and the second is systematic. In addition, first evidence is found for the modes $h_{c} \to 2(\pi{+}\pi{-})\pi{0}\eta$ and $h_{c}\to2(\pi{+}\pi{-})\omega$ with significances of 4.8$\sigma$ and 4.7$\sigma$, and their branching fractions are determined to be $(7.55\pm1.51\pm0.77)\times10{-3}$ and $\left( {4.00 \pm 0.86 \pm 0.35}\right) \times {10{ - 3}}$, respectively. No significant signals of $h_c\to 2(\pi+\pi-)\eta$ and $h_{c}\to p\bar{p}$ are observed, and the upper limits of the branching fractions of these decays are determined to be $<6.19\times10{-4}$ and $<4.40\times10{-5}$ at the 90% confidence level, respectively.
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