$\tau \to f_1 (1285)\pi^{-} \nu_{\tau}$ decay in the extended Nambu -- Jona-Lasinio model

TL;DR

This paper calculates the decay rate and invariant mass distribution for tau decay into f1(1285) pi nu using an extended Nambu-Jona-Lasinio model, including resonance contributions, and finds results consistent with experimental data.

Contribution

It introduces a detailed calculation of tau decay into f1(1285) pi nu within the extended NJL model, considering resonance exchanges and pi-a1 transitions, providing predictions aligned with experiments.

Findings

Estimated branching ratio: 4.0×10⁻⁴.

Distribution shows a clear a1(1640) resonance signal.

Predicted decay width of a1(1640) to f1 pi: 14.1 MeV.

Abstract

Within the framework of the extended Nambu -- Jona-Lasinio model, we calculate the matrix element of the $\tau \to f_1(1285) \pi^{-} \nu_{\tau}$ decay, obtain the invariant mass distribution of the $f_1\pi$ -system and estimate the branching ratio Br$(\tau \to f_1 \pi^{-}\nu_{\tau})=4.0\times 10^{-4}$. The two types of contributions are considered: the contact interaction, and the axial-vector $I^G(J^{PC})=1^-(1^{++})$ resonance exchange. The latter includes the ground $a_1(1260)$ state, and its first radially excited state, $a_1(1640)$. The corrections caused by the $\pi -a_1$ transitions are taken into account. Our estimate is in a good agreement with the latest empirical result Br$(\tau \to f_1 \pi^{-} \nu_{\tau})=(3.9\pm 0.5)\times 10^{-4}$. The distribution function obtained for the decay $\tau \to f_1(1285) \pi^{-} \nu_{\tau}$ shows a clear signal of $a_1(1640)$ resonance which should be compared with future experimental data including our estimate of the decay width $\Gamma (a_1(1640) \to f_1 \pi )=14.1\,\mbox{MeV}$.