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The radiative return at phi- and B-factories: FSR for muon pair production at next-to-leading order

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arxiv hep-ph/0404078 v2 pith:F2TT2MQ5 submitted 2004-04-08 hep-ph

classification hep-ph
keywords generatorproductionradiativecorrectionsintroducedmeasurementmuonnext-to-leading
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Muon pair production through the radiative return is of importance for a measurement of the hadronic production cross section in two ways: it provides an independent calibration and it may give rise to an important background for a measurement of the pion form factor. With this motivation the Monte Carlo event generator PHOKHARA is extended to include next-to-leading order radiative corrections to the reaction $e^+e^-\to \mu^+\mu^-\gamma$. Furthermore, virtual ISR corrections to FSR from pions are introduced, which extends the applicability of the generator into a new kinematical regime. Finally, the effect of photon vacuum polarization is introduced into this new version of the generator.

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Forward citations

Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. OpenAlex reports about 89 citations worldwide. Full citation record

  1. Soft QED as Open Quantum System: Infrared Cancellation and Soft-Shell Coarse Graining

    hep-th 2026-06 unverdicted novelty 7.0 of 10

    Formulates unresolved soft photons in QED as an open quantum system environment, derives IR-finite probabilities via influence functional and equal-history identity, and obtains explicit leading-soft Lindblad evolutio...

  2. Lepton anomalous magnetic moments: Theory

    hep-ph 2025-12 unverdicted novelty 2.0 of 10

    The paper provides an overview of theoretical calculations for lepton anomalous magnetic moments arising from quantum corrections in the Standard Model.

  3. The anomalous magnetic moment of the muon in the Standard Model

    hep-ph 2020-06 accept novelty 2.0 of 10

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

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