Annihilation Rates of Heavy 1−−1^{--} S-wave Quarkonia in Salpeter Method

preprint2010arXivOpen access

Abstract

The annihilation rates of vector 1−−1^{--} charmonium and bottomonium 3S1^3S_1 states V→e+e−V \rightarrow e^+e^- and V→3γV\rightarrow 3γ, V→γggV \rightarrow γgg and V→3gV \rightarrow 3g are estimated in the relativistic Salpeter method. We obtained Γ(J/ψ→3γ)=6.8×10−4Γ(J/ψ\rightarrow 3γ)=6.8\times 10^{-4} keV, Γ(ψ(2S)→3γ)=2.5×10−4Γ(ψ(2S)\rightarrow 3γ)=2.5\times 10^{-4} keV, Γ(ψ(3S)→3γ)=1.7×10−4Γ(ψ(3S)\rightarrow 3γ)=1.7\times 10^{-4} keV, Γ(Υ(1S)→3γ)=1.5×10−5Γ(Υ(1S)\rightarrow 3γ)=1.5\times 10^{-5} keV, Γ(Υ(2S)→3γ)=5.7×10−6Γ(Υ(2S)\rightarrow 3γ)=5.7\times 10^{-6} keV, Γ(Υ(3S)→3γ)=3.5×10−6Γ(Υ(3S)\rightarrow 3γ)=3.5\times 10^{-6} keV and Γ(Υ(4S)→3γ)=2.6×10−6Γ(Υ(4S)\rightarrow 3γ)=2.6\times 10^{-6} keV. In our calculations, special attention is paid to the relativistic correction, which is important and can not be ignored for excited 2S2S, 3S3S and higher excited states.

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