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Parity-violating Møller scattering: complete two-loop corrections
Abstract
The MOLLER experiment will measure the parity-violating asymmetry of Møller scattering to 2.4%. We present its fermionic and bosonic two-loop electroweak corrections to the zeroth and first orders in 1−4sin2θW. Light quarks enter through vacuum polarization from e+e- data or lattice QCD. For sin2θ̂W(MZ) = 0.23122 and an 11 GeV beam, the weak charge of the electron is $0.04546(8)$ (data) or 0.04517(5) (lattice). Two-loop terms contribute 1.5% of it. Uncomputed terms are estimated at 4% of the experimental goal; the data-lattice difference, about 25% of that goal, limits the prediction.
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BibTeX
@misc{czarnecki2026parityviolating,
title = {{Parity-violating Møller scattering: complete two-loop corrections}},
author = {Andrzej Czarnecki},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.40247},
eprint = {2610.40247},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.40247},
}
RIS
TY - UNPB
TI - Parity-violating Møller scattering: complete two-loop corrections
AU - Andrzej Czarnecki
PY - 2026
DA - 2026/10/29
PB - arXiv
DO - 10.48550/arxiv.2610.40247
UR - https://arxiv.org/abs/2610.40247
AB - The MOLLER experiment will measure the parity-violating asymmetry of Møller scattering to 2.4%. We present its fermionic and bosonic two-loop electroweak corrections to the zeroth and first orders in 1−4sin^2θ_W. Light quarks enter through vacuum polarization from e^+e^- data or lattice QCD. For sin^2θ̂_W(M_Z) = 0.23122 and an 11 GeV beam, the weak charge of the electron is $0.04546(8)$ (data) or 0.04517(5) (lattice). Two-loop terms contribute 1.5% of it. Uncomputed terms are estimated at 4% of the experimental goal; the data-lattice difference, about 25% of that goal, limits the prediction.
ER -