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Radiative corrections to $τ\toππν_τ$

Gilberto Colangelo, Martina Cottini, Martin Hoferichter, Simon Holz

TL;DR

The paper develops a dispersive, model-independent framework to compute radiative and isospin-breaking corrections to τ → ππν_τ, extending ChPT results with a pion-vector form factor that incorporates ρ, ρ′, and ρ″ resonances. By matching to ChPT and carefully treating real-emission contributions and endpoint/threshold singularities, they obtain a UV-finite, IR-consistent correction G_EM(s) and quantify the τ-specific IB corrections to a_mu^HVP,LO[ππ,τ], finding a notable ρ-region effect and a reduction in theoretical uncertainties, though scheme-matching with S_EW^{ππ} remains a dominant source of uncertainty. The work relies on fits to the τ spectral function using a dispersive f_+(s) with Omnès unitarization and conformal polynomials, enabling a coherent evaluation across the full kinematic range and highlighting tensions between threshold and resonance regions that motivate further data and lattice inputs. Overall, the analysis provides a more reliable long-range radiative correction for tau-based determinations of the two-pion HVP contribution to the muon g-2 and outlines the path toward a fully robust, data-driven HVP evaluation from hadronic τ decays.

Abstract

Hadronic $τ$ decays present an opportunity to determine the isovector part of the hadronic-vacuum-polarization contribution to the anomalous magnetic moment of the muon in a way complementary to $e^+e^-\to\text{hadrons}$ cross sections. However, the required isospin rotation is only exact in the isospin limit, and corrections need to be under control to draw robust conclusions, most notably for $τ\toππν_τ$ decays to determine the two-pion contribution, $a_μ^\text{HVP, LO}[ππ,τ]$. In this work, we present a novel analysis of the required radiative corrections using dispersion relations, thereby extending in a model-independent way the previous analysis in chiral perturbation theory (ChPT) beyond the threshold region. In particular, we include the dominant structure-dependent virtual corrections from pion-pole diagrams, leading to sizable changes in the vicinity of the $ρ(770)$ resonance. Moreover, we work out the matching to ChPT and devise a strategy for a stable numerical evaluation of real-emission contributions near the two-pion threshold, which proves important to capture isospin-breaking corrections enhanced by the threshold singularity. For the numerical analysis, we use a dispersive representation of the pion form factor including the $ρ'$, $ρ''$ resonances, perform fits to the available data sets for the $τ\toππν_τ$ spectral function, and calculate the corresponding radiative correction factor $G_\text{EM}(s)$ in a self-consistent manner. Based on these results, we evaluate the $τ$-specific isospin-breaking corrections to $a_μ^\text{HVP, LO}[ππ,τ]$.

Radiative corrections to $τ\toππν_τ$

TL;DR

The paper develops a dispersive, model-independent framework to compute radiative and isospin-breaking corrections to τ → ππν_τ, extending ChPT results with a pion-vector form factor that incorporates ρ, ρ′, and ρ″ resonances. By matching to ChPT and carefully treating real-emission contributions and endpoint/threshold singularities, they obtain a UV-finite, IR-consistent correction G_EM(s) and quantify the τ-specific IB corrections to a_mu^HVP,LO[ππ,τ], finding a notable ρ-region effect and a reduction in theoretical uncertainties, though scheme-matching with S_EW^{ππ} remains a dominant source of uncertainty. The work relies on fits to the τ spectral function using a dispersive f_+(s) with Omnès unitarization and conformal polynomials, enabling a coherent evaluation across the full kinematic range and highlighting tensions between threshold and resonance regions that motivate further data and lattice inputs. Overall, the analysis provides a more reliable long-range radiative correction for tau-based determinations of the two-pion HVP contribution to the muon g-2 and outlines the path toward a fully robust, data-driven HVP evaluation from hadronic τ decays.

Abstract

Hadronic decays present an opportunity to determine the isovector part of the hadronic-vacuum-polarization contribution to the anomalous magnetic moment of the muon in a way complementary to cross sections. However, the required isospin rotation is only exact in the isospin limit, and corrections need to be under control to draw robust conclusions, most notably for decays to determine the two-pion contribution, . In this work, we present a novel analysis of the required radiative corrections using dispersion relations, thereby extending in a model-independent way the previous analysis in chiral perturbation theory (ChPT) beyond the threshold region. In particular, we include the dominant structure-dependent virtual corrections from pion-pole diagrams, leading to sizable changes in the vicinity of the resonance. Moreover, we work out the matching to ChPT and devise a strategy for a stable numerical evaluation of real-emission contributions near the two-pion threshold, which proves important to capture isospin-breaking corrections enhanced by the threshold singularity. For the numerical analysis, we use a dispersive representation of the pion form factor including the , resonances, perform fits to the available data sets for the spectral function, and calculate the corresponding radiative correction factor in a self-consistent manner. Based on these results, we evaluate the -specific isospin-breaking corrections to .

Paper Structure

This paper contains 27 sections, 140 equations, 19 figures, 3 tables.

Figures (19)

  • Figure 1: Leading diagrams for the radiative corrections to $\tau^- (l_1) \to \pi^-(q_1) \pi^0(q_2) \nu_\tau(l_2)$, excluding wave-function renormalization.
  • Figure 2: Counterterm diagram for the radiative corrections to $\tau^- \to \pi^- \pi^0 \nu_\tau$.
  • Figure 3: Loop and counterterm diagrams of the external-leg contributions.
  • Figure 4: Triangle/box diagram with $\pi\pi\gamma$ and $\tau\nu_\tau\pi\pi$ vertices dressed with the pion VFF.
  • Figure 5: Initial- and final-state-radiations diagrams for $\tau^- \to \pi^- \pi^0 \nu_\tau$.
  • ...and 14 more figures