Study of χcJχ_{cJ} radiative decays into a vector meson

preprint2011arXivOpen access

Abstract

The decays χcJ→γVχ_{cJ}\toγV (V=ϕ,ρ0,ωV=ϕ, ρ^0, ω) are studied with a sample of radiative $\psip\toγχ_{cJ}$ events in a sample of $(1.06\pm0.04)\times 10^{8} \psip$ events collected with the BESIII detector. The branching fractions are determined to be: B(χc1→γϕ)=(25.8±5.2±2.3)×10−6{\cal B}(χ_{c1}\to γϕ)=(25.8\pm 5.2\pm 2.3)\times 10^{-6}, B(χc1→γρ0)=(228±13±22)×10−6{\cal B}(χ_{c1}\to γρ^0)=(228\pm 13\pm 22)\times 10^{-6}, and B(χc1→γω)=(69.7±7.2±6.6)×10−6{\cal B}(χ_{c1}\to γω)=(69.7\pm 7.2\pm 6.6)\times 10^{-6}. The decay χc1→γϕχ_{c1}\to γϕ is observed for the first time. Upper limits at the 90% confidence level on the branching fractions for χc0χ_{c0} and $\chict$ decays into these final states are determined. In addition, the fractions of the transverse polarization component of the vector meson in χc1→γVχ_{c1}\to γV decays are measured to be 0.29−0.12−0.09+0.13+0.100.29_{-0.12-0.09}^{+0.13+0.10} for χc1→γϕχ_{c1}\to γϕ, 0.158±0.034−0.014+0.0150.158\pm 0.034^{+0.015}_{-0.014} for χc1→γρ0χ_{c1}\to γρ^0, and 0.247−0.087−0.026+0.090+0.0440.247_{-0.087-0.026}^{+0.090+0.044} for χc1→γωχ_{c1}\to γω, respectively. The first errors are statistical and the second ones are systematic.

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