Abstract

In a combined study of the decay spectra of $\tau^-\to K_S\pi^-\nu_\tau$ and $\tau^-\to K^-\eta\nu_\tau$ decays within a dispersive representation of the required form factors, we illustrate how the $K^*(1410)$ resonance parameters, defined through the pole position in the complex plane, can be extracted with improved precision as compared to previous studies. While we obtain a substantial improvement in the mass, the uncertainty in the width is only slightly reduced, with the findings $M_{K^{*\prime}}=1304 \pm 17\,$MeV and $\Gamma_{K^{*\prime}} = 171 \pm 62\,$MeV. Further constraints on the width could result from updated analyses of the $K\pi$ and/or $K\eta$ spectra using the full Belle-I data sample. Prospects for Belle-II are also discussed. As the $K^-\pi^0$ vector form factor enters the description of the decay $\tau^-\to K^-\eta\nu_\tau$, we are in a position to investigate isospin violations in its parameters like the form factor slopes. In this respect also making available the spectrum of the transition $\tau^-\to K^-\pi^0\nu_\tau$ would be extremely useful, as it would allow to study those isospin violations with much higher precision.

Highlights

  • JHEP09(2014)042 positions and relative weight, the errors on the radial excitation were noticeably larger than in the K∗(892) case

  • In a combined study of the decay spectra of τ − → KSπ−ντ and τ − → K−ηντ decays within a dispersive representation of the required form factors, we illustrate how the K∗(1410) resonance parameters, defined through the pole position in the complex plane, can be extracted with improved precision as compared to previous studies

  • As the K−π0 vector form factor enters the description of the decay τ − → K−ηντ, we are in a position to investigate isospin violations in its parameters like the form factor slopes

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Summary

Form factor representations

The differential decay width of the transition τ − → KSπ−ντ as a function of the invariant mass of the two-meson system can be written as dΓ(τ −. While it is possible to obtain stable fits without using the KSπ− branching fraction as a data point, this is not the case for the K−η channel This is due to the fact that there are strong correlations between the branching ratio and the slope parameters of the vector form factor. Concerning the branching fractions, we observe that in the KSπ− channel our fit value BKπ, which is mainly driven by the explicit input, and the result when integrating the fitted spectrum BKthπ, are in very good agreement, pointing to a satisfactory description of the experimental data. The pole parameters of the K∗(892) resonance are in nice accord with previous values [15, 16] and have similar statistical fit uncertainties which is to be expected as these parameters are driven by the data of the τ − → KSπ−ντ decay, which was the process analysed previously. We mention that Belle-II statistics could be able to pinpoint possible inconsistencies between τ − → (Kπ)−ντ and τ − → K−ηντ data

Conclusions
A Exponential parametrisation of the vector form factor
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