Abstract

We study the processes $e^+e^-\to 2(\pi^+\pi^-)\pi^0\pi^0\pi^0\gamma$ and $2(\pi^+\pi^-)\pi^0\pi^0\eta\gamma$ in which an energetic photon is radiated from the initial state. The data were collected with the \babar~ detector at SLAC. About 14\,000 and 4700 events, respectively, are selected from a data sample corresponding to an integrated luminosity of 469 fb^{-1}. The invariant mass of the hadronic final state defines the effective \epem center-of-mass energy. The center-of-mass energies range from threshold to 4.5 GeV. From the mass spectra, the first ever measurements of the $e^+e^-\to 2(\pi^+\pi^-)\pi^0\pi^0\pi^0$ and the $e^+e^-\to2(\pi^+\pi^-)\pi^0\pi^0\eta$ cross sections are performed. The contributions from $\omega\pi^+\pi^-\pi^0\pi^0$, $\eta2(\pi^+\pi^-)$, and other intermediate states are presented. We observe the $J/\psi$ and $\psi(2S)$ in most of these final states and measure the corresponding branching fractions, many of them for the first time.

Highlights

  • The Standard Model (SM) calculation of the muon anomalous magnetic moment requires input from experimental eþe− hadronic cross section data in order to account for hadronic vacuum polarization terms

  • To evaluate the detector acceptance and efficiency, we have developed a special package of Monte Carlo (MC) simulation programs for radiative processes based on the approach of Kühn and Czyż [18]

  • The mass-dependent detection efficiency is obtained by dividing the number of fitted MC events in each 0.05 GeV=c2 mass interval of the hadronic system by the number generated in the same interval

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Summary

INTRODUCTION

The Standard Model (SM) calculation of the muon anomalous magnetic moment (gμ − 2) requires input from experimental eþe− hadronic cross section data in order to account for hadronic vacuum polarization terms. The calculation is most sensitive to the low-energy region, from the hadronic threshold to about 2 GeV, where the inclusive hadronic cross section cannot be measured reliably and a sum of exclusive states must be used. Measured, and new measurements will improve the reliability of the calculation These studies provide information on the resonant spectroscopy. The Xh studied to date include: charged hadron pairs πþπ− [4], KþK− [5], and pp [6]; four or six charged mesons [7,8,9]; charged mesons plus one or two or three π0 mesons [8,9,10,11,12,13]; a. We observe J=ψ and ψð2SÞ signals in the studied final states and the corresponding branching fractions are measured

THE BABAR DETECTOR AND DATASET
EVENT SELECTION AND KINEMATIC FIT
ADDITIONAL SELECTION CRITERIA
Number of signal events in simulation
Efficiency evaluation
Peaking background
Summary of systematic uncertainties
Overview of the intermediate structures
The ωπ0η intermediate state
The sum of intermediate states
Determination of the number of events
Findings
SUMMARY
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