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New precise measurement of the $e^+e^- \rightarrow π^+π^-(γ)$ cross section with BABAR

Léonard Polat

Abstract

The BABAR experiment participates to the global endeavor for a precise prediction of the anomalous magnetic moment of the muon by evaluating the contribution from hadronic vacuum polarization, in particular through cross section measurements of hadronic final states from $e^+e^-$ collisions. After a first measurement in 2009 of the largest input that comes from the $e^+e^- \rightarrow π^+π^-(γ)$ cross section, we present preliminary results from a new study on 460 ${\rm fb}^{-1}$ of BABAR data, involving a blind and independent procedure. The results of the two analyses are shown to be consistent.

New precise measurement of the $e^+e^- \rightarrow π^+π^-(γ)$ cross section with BABAR

Abstract

The BABAR experiment participates to the global endeavor for a precise prediction of the anomalous magnetic moment of the muon by evaluating the contribution from hadronic vacuum polarization, in particular through cross section measurements of hadronic final states from collisions. After a first measurement in 2009 of the largest input that comes from the cross section, we present preliminary results from a new study on 460 of BABAR data, involving a blind and independent procedure. The results of the two analyses are shown to be consistent.
Paper Structure (5 sections, 4 equations, 3 figures)

This paper contains 5 sections, 4 equations, 3 figures.

Figures (3)

  • Figure 1: The $\pi^+\pi^-$ contribution to $a_\mu$ in the energy range $0.6 < \sqrt{s} < 0.88$ GeV obtained from multiple experiments cmd (a) and comparison of dispersive predictions (preliminary new results in red) with the direct experimental measurement (vertical band) and lattice-based results (b).
  • Figure 2: Angular fit results in two $m_{\pi\pi}$ bins, close to threshold (a) and at the $\rho$ peak (b). The quantities $f_{XX\gamma}\ (X=\pi,\mu,K,e)$ give the fitted fractions of the relevant processes ($KK\gamma$ becomes negligible beyond 0.4 ${\rm GeV}/c^2$).
  • Figure 3: The $e^+e^- \rightarrow \pi^+\pi^-(\gamma)$ cross section measured in this work as a function of the reduced energy $\sqrt{s^\prime}$ (a) and the ratio of this measurement to the 2009 B A B A R result (b).