# The decays $\\tau \\to \\nu\_{\\tau} (K^{\*}(892), K^{\*}(1410), K\_1(1270), K\_1(1650), a\_1(1260), a\_1(1640))$ in the Extended Nambu-Jona-Lasinio Model

Source: [The decays $\\tau \\to \\nu\_{\\tau} (K^{\*}(892), K^{\*}(1410), K\_1(1270), K\_1(1650), a\_1(1260), a\_1(1640))$ in the Extended Nambu-Jona-Lasinio Model](<https://www.sota2.com/research/paper/68fa36771e209131ce8aa27e>)

Collection index: [llms.txt](<https://www.sota2.com/research/llms.txt>)

Data updated: 2025-10-24T21:51:16.544Z

Authors: M.K.Volkov, K. Nurlan

Published: 2016-12-27T17:02:26.000Z

## Abstract

The decays $\\tau \\to \\nu\_{\\tau} (K^{\*}(892), K^{\*}(1410), K\_1(1270), K\_1(1650), a\_1(1260), a\_1(1640))$ in the extended NJL model are calculated. The results obtained for the decays are $\\tau \\to \\nu\_{\\tau} (K^{\*}(892), K^{\*}(1410), K\_1(1270))$ in a satisfactory agreement with the experimental data. There are no experimental data for other types of decay. Therefore, the obtained results should be considered as predictions for further experiments.

## Recorded benchmark results

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## Original sources and implementation

[Original paper](<https://arxiv.org/abs/1612.08681>)

[PDF](<https://arxiv.org/pdf/1612.08681.pdf>)
