KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross section. These measurements are based on approximate NLO $ \mu^+ \mu^- \gamma $ cross section predictions of the Monte Carlo event generator PHOKHARA7.0. In this article, the complete NLO radiative corrections to $ \mu^+ \mu^- \gamma $ production are calculated and implemented in the Monte Carlo event generator PHOKHARA9.0. Numerical reliability is guaranteed by two independent approaches to the real and the virtual corrections. The novel features include the contribution of pentagon diagrams in the virtual corrections, which form a gauge-invariant set when combined with their box diagram partners. They may contribute to certain distributions...
The theoretical calculation of the leading quantum electrodynamics radiative corrections to the proc...
The complete one-loop QED initial state, final state and initial--final state interference correctio...
The measurement of the pion form factor and, more generally, of the cross section for electron–posit...
KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross ...
KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross ...
KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross ...
Muon pair production through the radiative return is of importance for a measurement of the hadronic...
ABSTRACT: The precise determination of the cross section for electron-positron annihilation into had...
Electron-positron annihilation into hadrons plus an energetic photon from initial state radiation al...
We present a NNLO QCD accurate event generator for direct photon pair production at hadron colliders...
The energy dependence of the electron - positron hadronic cross section can be measured not only by ...
We study predictions for the reaction $e^+e^- \to {\bar \nu} \nu (n \gamma)$. The complete one-loop ...
We study predictions for the reaction e"+e"- #-># anti #nu##nu#(n#gamma#). The complete...
Electron--positron annihilation into hadrons plus an energetic photon from initial-state radiation a...
The Monte Carlo event generator BabaYaga has been developed in the last decade for high precision si...
The theoretical calculation of the leading quantum electrodynamics radiative corrections to the proc...
The complete one-loop QED initial state, final state and initial--final state interference correctio...
The measurement of the pion form factor and, more generally, of the cross section for electron–posit...
KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross ...
KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross ...
KLOE and Babar have an observed discrepancy of 2% to 5% in the invariant pion pair production cross ...
Muon pair production through the radiative return is of importance for a measurement of the hadronic...
ABSTRACT: The precise determination of the cross section for electron-positron annihilation into had...
Electron-positron annihilation into hadrons plus an energetic photon from initial state radiation al...
We present a NNLO QCD accurate event generator for direct photon pair production at hadron colliders...
The energy dependence of the electron - positron hadronic cross section can be measured not only by ...
We study predictions for the reaction $e^+e^- \to {\bar \nu} \nu (n \gamma)$. The complete one-loop ...
We study predictions for the reaction e"+e"- #-># anti #nu##nu#(n#gamma#). The complete...
Electron--positron annihilation into hadrons plus an energetic photon from initial-state radiation a...
The Monte Carlo event generator BabaYaga has been developed in the last decade for high precision si...
The theoretical calculation of the leading quantum electrodynamics radiative corrections to the proc...
The complete one-loop QED initial state, final state and initial--final state interference correctio...
The measurement of the pion form factor and, more generally, of the cross section for electron–posit...