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The decays of $chi_{c2}to K^{+}K^{-}pi^{0}$, $K_{S} K^{pm}pi^{mp}$ and $pi^{+}pi^{-}pi^{0}$ are studied with the $psi(3686)$ data samples collected with the Beijing Spectrometer (BESIII). For the first time, the branching fractions of $chi_{c2}to K^{ast}overline{K}$, $chi_{c2}to a_{2}^{pm}(1320)pi^{mp}/a_{2}^{0}(1320)pi^{0}$ and $chi_{c2}to rho(770)^{pm}pi^{mp}$ are measured. Here $K^{ast}overline{K}$ denotes both $K^{astpm}K^{mp}$ and $K^{ast 0}overline{K}{}^{0}+c.c.$, and $K^{ast}$ denotes the resonances $K^{ast}(892)$, $K^{ast}_{2}(1430)$ and $K^{ast}_{3}(1780)$. The observations indicate a strong violation of the helicity selection rule in $chi_{c2}$ decays into vector and pseudoscalar meson pairs. The measured branching fractions of $chi_{c2}to K^{ast}(892)overline{K}$ are more than 10 times larger than the upper limit of $chi_{c2}to rho(770)^{pm}pi^{mp}$, which is so far the first direct observation of a significant $U$-spin symmetry breaking effect in charmonium decays.
Using a sample of $447.9times 10^6$ $psi(3686)$ events collected with the BESIII detector in 2009 and 2012, we study the decays $chi_{c0,2}to$ $etaeta$ and $etaeta$. The decays $chi_{c2}toetaeta$, $chi_{c0}toetaeta$ and $chi_{c2}toetaeta$ are observe
Based on a data sample of 106 M $psi^{prime}$ events collected with the BESIII detector, the decays $psi^{prime}argammachi_{c0, 2}$,$chi_{c0, 2}argammagamma$ are studied to determine the two-photon widths of the $chi_{c0, 2}$ states. The two-photon d
The $overline{B_s^0} rightarrow chi_{c2} K^+ K^- $ decay mode is observed and its branching fraction relative to the corresponding $chi_{c1}$ decay mode, in a $pm 15 textrm{MeV}/c^2$ window around the $phi$ mass, is found to be $frac{mathcal{B}(overl
Based on $448.1 times 10^6$ $psi(3686)$ events collected with the BESIII detector, the decays $psi(3686)togammachi_{cJ}, chi_{cJ} to gammagamma~(J=0, 1, 2)$ are studied. The decay branching fractions of $chi_{c0,c2} to gammagamma$ are measured to be
Decays $chi_{cJ}~(J=0,1,2)toomegaphi$ are studied using $(448.1pm2.9)times 10^{6} ~psi(3686)$ events collected with the BESIII detector in 2009 and 2012. In addition to the previously established $chi_{c0}toomegaphi$, first observation of $chi_{c1} t