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The \(\tau\rightarrow\bar{K}^{*0}(892)\pi^{-}\nu_\tau\) Decay in the Nambu–Jona-Lasinio Model

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Abstract

The width of the \(\tau\rightarrow\bar{K}^{*0}(892)\pi^{-}\nu_\tau\) decay is calculated within the Nambu–Jona-Lasinio model taking into account four channels of the formation of the \(\tau\rightarrow\bar{K}^{*0}(892)\pi^{-}\) pair—the contact interaction and three channels with intermediate axial-vector, vector, and pseudoscalar mesons. Leading contributions arise from the contact interaction and axial-vector channel with an intermediate ground-state K1(1270) meson. Our theoretical estimate adequately reproduces the measured \(\tau\rightarrow\bar{K}^{*0}(892)\pi^{-}\nu_\tau\) decay width.

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Correspondence to M. K. Volkov.

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Original Russian Text © M.K. Volkov, A.A. Pivovarov, 2018, published in Pis’ma v Zhurnal Eksperimental’noi i Teoreticheskoi Fiziki, 2018, Vol. 108, No. 6, pp. 369–373.

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Volkov, M.K., Pivovarov, A.A. The \(\tau\rightarrow\bar{K}^{*0}(892)\pi^{-}\nu_\tau\) Decay in the Nambu–Jona-Lasinio Model. Jetp Lett. 108, 347–351 (2018). https://doi.org/10.1134/S0021364018180145

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  • DOI: https://doi.org/10.1134/S0021364018180145

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