Abstract

We present the fully up-to-date calculation of the $\gamma Z$-box correction which needs to be taken into account to determine the weak mixing angle at low energies from parity-violating electron proton scattering. We make use of neutrino and antineutrino inclusive scattering data to predict the parity-violating structure function $F_3^{\gamma Z}$ by isospin symmetry. Our new analysis confirms previous results for the axial contribution to the $\gamma Z$-box graph, and reduces the uncertainty by a factor of~2. In addition, we note that the presence of parity-violating photon-hadron interactions induces an additional contribution via $F_3^{\gamma \gamma}$. Using experimental and theoretical constraints on the nucleon anapole moment we are able to estimate the uncertainty associated with this contribution. We point out that future measurements are expected to significantly reduce this latter uncertainty.

Highlights

  • The precision measurement of s2W ≡ sin2 θW, where θW is the Standard Model (SM) weak mixing angle, in parityviolating (PV) electron scattering serves as a powerful tool to test the SM and search for physics beyond it

  • We present the fully up-to-date calculation of the γZ-box correction which needs to be taken into account to determine the weak mixing angle at low energies from parity-violating electron proton scattering

  • Since the energy dependence of s2W is very precisely predicted within the SM [1], any significant deviation from it would be an indication of beyond Standard Model (BSM) physics

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Summary

INTRODUCTION

The precision measurement of s2W ≡ sin θW, where θW is the Standard Model (SM) weak mixing angle, in parityviolating (PV) electron scattering serves as a powerful tool to test the SM and search for physics beyond it. Since the energy dependence of s2W is very precisely predicted within the SM [1], any significant deviation from it would be an indication of beyond Standard Model (BSM) physics. DσÆ are the differential cross sections for scattering with right-handed and left-handed polarized electrons, respectively. At tree level this quantity is given by 1 − 4s2W, which is accidentally suppressed. This effectively leads to an enhancement in the sensitivity to s2W, Δs2W s2W

ΔQpW QpW
Published by the American Physical Society
Re ln
We visualize the source of this uncertainty reduction in
Elastic DIS Nπ Resonances Regge
The elastic
Findings
SUMMARY AND CONCLUSIONS
Full Text
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