The quark axial vector coupling and heavy meson decays

preprint1995arXivOpen access

Abstract

Form factors and decay widths for D∗→DγD^{\ast}\rightarrow D γ and D∗→DπD^{\ast}\rightarrow D π decays are estimated in a relativistic constituent quark model. Relativistic corrections due to light quarks are found to be substantial and to suppress the vector and axial vector form factors. The CLEO experimental value of Rγ0≡Γ(D∗0→D0γ)/Γ(D∗0→D0π0)=0.572±0.057±0.081R^0_γ\equiv Γ(D^{\ast 0}\rightarrow D^{0} γ)/ Γ(D^{\ast 0}\rightarrow D^{0} π^{0})=0.572\pm 0.057\pm 0.081 is used to determine the quark axial vector coupling gAg_A, which is found to be 0.6−0.80.6-0.8 for mu=(350−200)MeVm_u=(350-200) MeV correspondingly, as compared with the chiral model result gA=0.8−0.9g_{A}= 0.8-0.9. The heavy meson-pion strong coupling gg is found to be 0.4−0.60.4-0.6, much smaller than g=1g=1 which is expected in the large NCN_{C} and nonrelativistic limit, but consistent with some heavy hadron chiral theory and QCD sum rule results. The failure of nonrelativistic treatment for the light quark in the heavy meson decays is also emphasized.

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