Abstract
The width of the \(\tau\rightarrow\bar{K}^{0*}(892)\pi^-\nu_\tau\) decay has been calculated within the extended Nambu-Jona-Lasinio model taking into account intermediate axial-vector, vector, and pseudoscalar mesons in the ground and first radially excited states. The splitting of the axial-vector intermediate state K1A into two physical mesons K1(1270) and K1(1400) caused by the mixing of axial-vector strange mesons from the 3P1 and 1P1 nonets has also been taken into account. The results are in satisfactory agreement with experimental data.
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