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Revisit of the electromagnetic correction to $τ\toππν_τ$ and its implication for muon $g-2$ based on $τ$ data

Zhi-Xin Li, Ao Li, Jin Hao, Chun-Gui Duan, Zhi-Hui Guo

TL;DR

The paper revisits the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment $a_{\mu}$ from the $\pi\pi$ channel by exploiting experimental $\tau\to\pi\pi\nu_{\tau}$ data and a refined long-distance electromagnetic correction $G_{\rm EM}$. It computes $G_{\rm EM}$ from the full $\tau^-\to\pi^-\pi^0\nu_\tau\gamma$ amplitude within resonance chiral theory, including both even- and odd-intrinsic-parity resonance operators, and determines the resonance coupling $d_4$ by analyzing $\omega\to\pi^0\pi^0\gamma$ with both vector and scalar resonances; two solutions emerge, Sol-A with $d_4=-0.42$ and Sol-B with $d_4=1.01$. The negative solution aligns with previous $O(p^4)$ results, while the positive solution aligns with some $O(p^6)$ findings, and the authors adopt Sol-A as the baseline, treating the difference as a systematic. Using the complete isospin-breaking corrections in $R_{\rm IB}(t)$ and the tau data from Belle, ALEPH, CLEO, and OPAL, they obtain $a_{\mu}^{\rm HVP,LO}|_{\pi\pi,\tau\text{data}} = 516.0(5.4)\times 10^{-10}$ and, when combined with other hadronic channels, $a_{\mu}^{\rm HVP,LO}|_{\tau\text{data}} = 702.1(5.4)\times 10^{-10}$; after incorporating the WP25 updates, the implied SM deviation is $\Delta a_{\mu} = (14.9 \pm 5.6)\times 10^{-10}$, corresponding to about $2.7\sigma$. The analysis demonstrates the sensitivity of the EM corrections to the $d_4$ parameter and provides an independent cross-check of the $a_{\mu}$ evaluation using $\tau$ data, highlighting a remaining tension with the current world average.

Abstract

In this work we focus on the evaluation of the leading-order hadronic vacuum polarization contribution from the $ππ$ channel to the muon anomalous magnetic moment $a_μ$ by using the experimental $τ\toππν_τ$ data. The isospin breaking corrections play the decisive role in this approach of computing $a_μ$. One of such important isospin breaking sources is the long-distance electromagnetic correction factor $G_{\rm EM}$ of the $τ\toππν_τ$ process from the real photon radiation. The latter effect can be calculated from the $τ\toππν_τγ$ amplitude, which is revised in this work within the resonance chiral theory by simultaneously including the even-intrinsic-parity and odd-intrinsic-parity resonance operators. We update the determination of the only unknown resonance coupling through the $ω\toπ^0π^0γ$ decay by including contributions from both the vector and scalar resonances. By taking other remaining contributions from the muon $g-2$ White Paper 2025, we further revise the complete value of $a_μ$, which turns out to deviate from the newest world average result after Fermilab's measurement at the level of 2.7 $σ$.

Revisit of the electromagnetic correction to $τ\toππν_τ$ and its implication for muon $g-2$ based on $τ$ data

TL;DR

The paper revisits the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment from the channel by exploiting experimental data and a refined long-distance electromagnetic correction . It computes from the full amplitude within resonance chiral theory, including both even- and odd-intrinsic-parity resonance operators, and determines the resonance coupling by analyzing with both vector and scalar resonances; two solutions emerge, Sol-A with and Sol-B with . The negative solution aligns with previous results, while the positive solution aligns with some findings, and the authors adopt Sol-A as the baseline, treating the difference as a systematic. Using the complete isospin-breaking corrections in and the tau data from Belle, ALEPH, CLEO, and OPAL, they obtain and, when combined with other hadronic channels, ; after incorporating the WP25 updates, the implied SM deviation is , corresponding to about . The analysis demonstrates the sensitivity of the EM corrections to the parameter and provides an independent cross-check of the evaluation using data, highlighting a remaining tension with the current world average.

Abstract

In this work we focus on the evaluation of the leading-order hadronic vacuum polarization contribution from the channel to the muon anomalous magnetic moment by using the experimental data. The isospin breaking corrections play the decisive role in this approach of computing . One of such important isospin breaking sources is the long-distance electromagnetic correction factor of the process from the real photon radiation. The latter effect can be calculated from the amplitude, which is revised in this work within the resonance chiral theory by simultaneously including the even-intrinsic-parity and odd-intrinsic-parity resonance operators. We update the determination of the only unknown resonance coupling through the decay by including contributions from both the vector and scalar resonances. By taking other remaining contributions from the muon White Paper 2025, we further revise the complete value of , which turns out to deviate from the newest world average result after Fermilab's measurement at the level of 2.7 .

Paper Structure

This paper contains 5 sections, 58 equations, 3 figures, 3 tables.

Figures (3)

  • Figure 1: Illustration of relevant Feynman diagrams for the scalar resonance contribution to the $\omega\to\pi^0\pi^0\gamma$ decay. The thick solid black line and the wiggle line denote the $\omega$ resonance and the photon, respectively, while the dashed lines stand for the pions.
  • Figure 2: Illustration of different results for EM corrected function $G_{\text{EM}}(t)$: Sol-A (black dashed line, with negative value of $d_4$), Sol-B (orange dashed line, with positive value of $d_4$), $G_{\text{EM}}^{\text{SI}}(t)$ (red long-dashed line, SI term only), the leading Low approximation for $G_{\text{EM}}^{(0)}(t)$ (blue dotted line) and the result with the full amplitude from Ref. Cirigliano:2002pv (blue solid line, labeled as CEN).
  • Figure 3: Full IB correction functions $R_{\text{IB}}(t)$ with complete EM corrections $G_{\text{EM}}\left(t\right)$.