EM Decay of X(3872) as the 11D2(2−+)1{^1D_2}(2^{-+}) charmonium

preprint2012arXivOpen access

Abstract

The recently BaBar results raise the possibility that X(3872) has negative parity. This makes people reconsider assigning X(3872) to the 11D2(ccˉ)1{^1D_2}(c\bar c) state. In this paper we give a general form of the wave function of 2−+2^{-+} mesons. By solving the instantaneous Bethe-Salpeter equation, we get the mass spectrum and corresponding wave functions. We calculate electromagnetic decay widths of the first 2−+2^{-+} state which we assume to be the X(3872) particle. The results are Γ(2−+(3872)→J/ψγ)=1.59−0.42+0.53Γ(2^{-+}(3872)\rightarrow J/ψγ) = 1.59^{+0.53}_{-0.42} keV, Γ(2−+(3872)→ψ(2S)γ)=2.87−0.97+1.46Γ(2^{-+}(3872)\rightarrow ψ(2S)γ) = 2.87^{+1.46}_{-0.97} eV and Γ(2−+(3872)→ψ(3770)γ)=0.135−0.047+0.066Γ(2^{-+}(3872)\rightarrow ψ(3770)γ) = 0.135^{+0.066}_{-0.047} keV. The ratio of branch fractions of the second and first channel is about 0.002, which is inconsistent with the experimental value 3.4±1.43.4\pm 1.4. So X(3872) is unlikely to be a 2−+2^{-+} charmonium state. In addition, we obtain a relatively large decay width for 2−+(3872)→hcγ2^{-+}(3872)\rightarrow h_cγ channel which is 392−111+62392^{+62}_{-111} keV.

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