Abstract

We combine ALEPH and OPAL results for the spectral distributions measured in $\tau\to\pi^-\pi^0\nu_\tau$, $\tau\to 2\pi^-\pi^+\pi^0\nu_\tau$ and $\tau\to\pi^-3\pi^0\nu_\tau$ decays with (i) recent BaBar results for the analogous $\tau\to K^- K^0\nu_\tau$ distribution and (ii) estimates of the contributions from other hadronic $\tau$-decay modes obtained using CVC and electroproduction data, to obtain a new and more precise non-strange, inclusive vector, isovector spectral function. The BaBar $K^- K^0$ and CVC/electroproduction results provide us with alternate, entirely data-based input for the contributions of all exclusive modes for which ALEPH and OPAL employed Monte-Carlo-based estimates. We use the resulting spectral function to determine $\alpha_s(m_\tau)$, the strong coupling at the $\tau$ mass scale, employing finite energy sum rules. Using the fixed-order perturbation theory (FOPT) prescription, we find $\alpha_s(m_\tau)=0.3077\pm 0.0075$, which corresponds to the five-flavor result $\alpha_s(M_Z)=0.1171\pm 0.0010$ at the $Z$ mass. While we also provide an estimate using contour-improved perturbation theory (CIPT), we point out that the FOPT prescription is to be preferred for comparison with other $\alpha_s$ determinations employing the $\overline{{\rm MS}}$ scheme, especially given the inconsistency between CIPT and the standard operator product expansion recently pointed out in the literature. Additional experimental input on the dominant $2\pi$ and $4\pi$ modes would allow for further improvements to the current analysis.

Highlights

  • Since the calculation of the term of order α4s in the Adler function [1], there has been a revived interest in the determination of the strong coupling, αsðmτÞ, at the τ mass scale mτ, from nonstrange hadronic τ decays

  • While we provide an estimate using contour-improved perturbation theory (CIPT), we point out that the fixed-order perturbation theory (FOPT) prescription is to be preferred for comparison with other αs determinations employing the MS scheme, especially given the inconsistency between CIPT and the standard operator product expansion recently pointed out in the literature

  • II C we argue that fixed-order perturbation theory (FOPT) should be favored over contour-improved perturbation theory (CIPT) [28,29], if the goal is to convert our result for αsðmτÞ to a value at the Z mass to be compared to MS values of αsðMZÞ obtained from other sources

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Summary

INTRODUCTION

Since the calculation of the term of order α4s in the Adler function [1], there has been a revived interest in the determination of the strong coupling, αsðmτÞ, at the τ mass scale mτ, from nonstrange hadronic τ decays. We combine, and update, the results for the contributions from the exclusive modes for which ALEPH and OPAL data is publicly available (the dominant 2π and 4π modes), using the method employed to combine exclusive-mode eþe− → hadrons RðsÞ data from different experiments and described in detail in Ref.

THEORY OVERVIEW
Finite energy sum rules
Choice of weight functions and the OPE
Perturbative uncertainties and FOPT vs CIPT
External input
NX dNXðsÞ ds ð3:2Þ where
Combining the ALEPH and OPAL 2π and 4π data
Residual mode updates
The KKπ contribution
The 6π contributions
The KKππ contributions
The inclusive V nonstrange spectral function
THE STRONG COUPLING
Strategy
Results
Analysis
Findings
CONCLUSION
Full Text
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