Test of Quantum Electrodynamics by Electron-Electron Scattering
William C. Barber, Gerard K. O'Neill, B. Gittelman, B. Richter
Abstract
William C. Barber, Gerard K. O'Neill, B. Gittelman, B. Richter
Abstract
We have measured the differential cross section for electron-electron scattering at a total energy of 1112 MeV in the center-of-mass system. Using the Feynman regulator as a model for violation, with $K$ a cutoff momentum, we find ${K}^{\ensuremath{-}2}=0.044\ifmmode\pm\else\textpm\fi{}0.049 {(\frac{\mathrm{GeV}}{c})}^{\ensuremath{-}2}$. The error quoted represents a statistical contribution of \ifmmode\pm\else\textpm\fi{}0.042 combined in quadrature with \ifmmode\pm\else\textpm\fi{}0.025 representing the uncertainty of possible systematic contributions. This result is one of the most sensitive high-momentum-transfer tests of the photon propagator in quantum electrodynamics.
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We have measured the differential cross section for electron-electron scattering at a total energy of 1112 MeV in the center-of-mass system. Using the Feynman regulator as a model for violation, with $K$ a cutoff momentum, we find ${K}^{\ensuremath{-}2}=0.044\ifmmode\pm\else\textpm\fi{}0.049 {(\frac{\mathrm{GeV}}{c})}^{\ensuremath{-}2}$. The error quoted represents a statistical contribution of \ifmmode\pm\else\textpm\fi{}0.042 combined in quadrature with \ifmmode\pm\else\textpm\fi{}0.025 representing the uncertainty of possible systematic contributions. This result is one of the most sensitive high-momentum-transfer tests of the photon propagator in quantum electrodynamics.
Key concepts: Physics, Propagator, Electron, Photon, Scattering, Quantum electrodynamics, Momentum (technical analysis), Feynman diagram