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The radiative return at phi- and B-factories: FSR at next-to-leading order

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
abstract

The measurement of the pion form factor and, more generally, of the cross section for electron--positron annihilation into hadrons through the radiative return has become an important task for high luminosity colliders such as the $\Phi$- or $B$-meson factories. For detailed understanding and analysis of this reaction, the construction of a Monte Carlo program, PHOKHARA, has been undertaken. Version 2.0 was based on a next-to-leading order (NLO) treatment of the corrections from initial-state radiation (ISR). In the present paper a further extension of PHOKHARA (version 3.0) is described, which incorporates NLO corrections to final-state radiation (FSR). The impact of combined ISR and FSR on various distributions is investigated and methods are presented, which will allow the extraction of the form factor, and even give access to inclusive photon emission due to FSR. The dependence of the results on the model for FSR is discussed and the impact of this contribution on the anomalous magnetic moment of the muon is evaluated.

citation-role summary

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hep-ph 2

years

2025 1 2020 1

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representative citing papers

Disperon QED

hep-ph · 2025-12-11 · unverdicted · novelty 6.0

Disperon QED is a new technique that feeds experimental data into higher-order QED loop calculations in Monte Carlo generators via dispersion relations and threshold subtraction.

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Showing 2 of 2 citing papers.

  • Disperon QED hep-ph · 2025-12-11 · unverdicted · none · ref 57 · internal anchor

    Disperon QED is a new technique that feeds experimental data into higher-order QED loop calculations in Monte Carlo generators via dispersion relations and threshold subtraction.

  • The anomalous magnetic moment of the muon in the Standard Model hep-ph · 2020-06-08 · accept · none · ref 197 · internal anchor

    The Standard Model value for the muon anomalous magnetic moment is 116591810(43)×10^{-11}, 3.7σ below the Brookhaven experimental measurement.