PreprintCC BY 4.0arXiv
The γZ-box correction and its impact on parity-violating deep-inelastic scattering
Abstract
The γZ-box correction is an important electroweak contribution to precision parity-violation measurements, but its conventional low-energy treatment relies on an ambiguous effective quark-mass prescription. We revisit this correction using a finite-mass calculation that provides a well-defined perturbative contribution without introducing such an auxiliary scale. Applying the result to the Jefferson Lab PVDIS measurement shifts the extracted electron-quark couplings at the 10−3 level. We discuss the implications of this shift for precision electroweak tests and the need for a consistent separation of perturbative and non-perturbative hadronic contributions.
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BibTeX
@misc{duch2026γzbox,
title = {{The $γZ$-box correction and its impact on parity-violating deep-inelastic scattering}},
author = {Balma Duch and Pere Masjuan and Hubert Spiesberger},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.15181},
eprint = {2609.15181},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.15181},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - The γZ-box correction and its impact on parity-violating deep-inelastic scattering
AU - Balma Duch
AU - Pere Masjuan
AU - Hubert Spiesberger
PY - 2026
DA - 2026/09/14
PB - arXiv
DO - 10.48550/arxiv.2609.15181
UR - https://arxiv.org/abs/2609.15181
AB - The γZ-box correction is an important electroweak contribution to precision parity-violation measurements, but its conventional low-energy treatment relies on an ambiguous effective quark-mass prescription. We revisit this correction using a finite-mass calculation that provides a well-defined perturbative contribution without introducing such an auxiliary scale. Applying the result to the Jefferson Lab PVDIS measurement shifts the extracted electron-quark couplings at the 10^−3 level. We discuss the implications of this shift for precision electroweak tests and the need for a consistent separation of perturbative and non-perturbative hadronic contributions.
ER -