Polynomial kernels with zeros at the radial excitation masses are used to suppress the hadronic continuum in QCD sum rules, giving B_K ≈ 0.91, B_B ≈ 1.0, m0² ≈ 1.0 GeV², and f_K ≈ 0.107 GeV.
The decays $\tau\rightarrow (K, K(1460))\nu_{\tau}$ and the value of the weak decay coefficients ${F}_{K}$ and ${{F}_{{K}^{'}}}$ in the extended NJL model
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abstract
In the extended NJL model, the decay widths of $\tau\rightarrow (K, K(1460))\nu_{\tau}$, $(K, K(1460))\rightarrow {\mu}\nu_{\mu}$ are calculated. The contributions from intermediate axial-vector mesons ${K}_{1}(1270)$, ${K}_{1}(1400)$ and the first radially excited state ${K}_{1}(1650)$ are taken into account. Estimates for the weak decay coefficients ${F}_{K}$ and ${{F}_{{K}^{'}}}$ are given. Predictions are made for the width of $\tau\rightarrow K(1460)\nu_{\tau}$ decay and ${{F}_{{K}^{'}}}$ constant.
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Pseudoscalar Meson Mixing, the Contribution of the Hadronic Continuum to Deviation from Factorization
Polynomial kernels with zeros at the radial excitation masses are used to suppress the hadronic continuum in QCD sum rules, giving B_K ≈ 0.91, B_B ≈ 1.0, m0² ≈ 1.0 GeV², and f_K ≈ 0.107 GeV.