The $Q_{weak}$ Experiment: First Determination of the Weak Charge of the Proton

TL;DR

The $Q_{weak}$ experiment measured the parity-violating asymmetry in electron-proton scattering to determine the proton's weak charge, providing a precise test of the Standard Model and constraints on new physics.

Contribution

First measurement of the weak charge of the proton using parity-violating electron scattering at low momentum transfer.

Findings

Measured asymmetry: -279 ± 35 (stat) ± 31 (syst) ppb

Determined $Q_W^p$ (PVES) = 0.064 ± 0.012 in agreement with SM

Extracted weak charges of up and down quarks from combined data

Abstract

The $Q_{weak}$ Collaboration has completed a challenging measurement of the parity-violating asymmetry in elastic electron-proton ($\vec{e}$p) scattering at the Thomas Jefferson National Accelerator Facility (Jefferson Lab). The initial result reported here is extracted from the commissioning part of the experiment, constituting about 4% of the full data set. The parity-violating asymmetry at a low momentum transfer $Q^2$=0.025 GeV$^2$ is $A_{ep}$ = -279 $\pm$ 35 (stat) $\pm$ 31 (syst) ppb, which is the smallest and most precise asymmetry ever measured in $\vec{e}$p scattering. This result allowed the first determination of the weak charge of the proton $Q_W^p$ from a global fit of parity-violating elastic scattering (PVES) results from nuclear targets, where earlier data at higher $Q^2$ constrain uncertainties of hadronic structure. The value extracted from the global fit is $Q_W^p$ (PVES) = 0.064 $\pm$ 0.012, in agreement with the standard model prediction $Q_W^p$ (SM) = 0.0710 $\pm$ 0.0007. The neutral weak charges of up and down quarks are extracted from a combined fit of the PVES results with a previous atomic parity violation (APV) measurement on $^{133}$Cs. The analysis of the full $Q_{weak}$ data is ongoing and expected to yield a value for the asymmetry within 10 ppb of precision. Because of the suppression of $Q_W^p$, such a high precision measurement will place significant constraints to models of physics beyond the standard model.