The decay τ→K∗−(892)ηνττ\to K^{*-}(892) ην_τ in the NJL model

preprint2019arXivOpen access

Abstract

The decay width τ→K∗−(892)ηνττ\to K^{*-}(892) ην_τ was calculated in the Nambu--Jona-Lasinio model. Four channels were taken into account: the contact channel (the final states are directly producted from lepton current without any intermediate meson states), the axial-vector channel with two intermediate physical states K1(1270)K_{1}(1270) and K1(1400)K_{1}(1400), the vector channel with intermediate K∗(892)K^{*}(892) meson and the pseudoscalar channel with intermediate KK meson. It is shown that the first two channels give the dominant contribution to the decay width. Of the remaining two channels, the pseudoscalar channel plays a more prominent role. The final result is in satisfactory agreement with experimental data. Prediction for the differential decay width is presented.

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