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In the extended Nambu–Jona-Lasinio model, the decay widths of the processes were calculated. The intermediate strange quark-antiquark mesons in both the ground and the first radially excited states were taken into account. The meson , being a possible candidate for the role of the tetraquark meson, was also taken into account as an intermediate state. The result for the process $\tau \to \omega(782) K^{-} \nu_{\tau}$ is in satisfactory agreement with the experimental data. Simultaneously, the result for the decay $\tau \to \phi(1020) K^{-} \nu_{\tau}$ is in agreement with the experimental data with precision .

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