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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  -