Parity-Violating and Parity-Conserving Asymmetries in \boldmath$\vec{e}p$ and \boldmath$\vec{e}N$ Scattering in the Qweak Experiment*

The Qweak experiment at Jefferson Lab has made the first determination of the weak charge of the proton in elastic scattering of longitudinally polarized electrons from unpolarized protons at a momentum transfer $Q^2$ of 0.025 (GeV/c)$^2$. To achieve the required precision to measure the small parity-violating asymmetry of -279 parts per billion, we directed a 180 $\mu$A 85\%-polarized electron beam on a 35 cm long liquid hydrogen target and integrated scattered events in eight azimuthally symmetric fused silica Cerenkov detectors. Based on 4\% of the total data collected by the experiment, we find a value for the weak charge of proton in agreement with predictions of the Standard Model. To correct for the contributions from background processes, we conducted several additional parity-violating and parity-conserving asymmetry measurements with different kinematics (elastic and $N \to \Delta$), electron polarization (longitudinal and transverse), and targets (protons, electrons, aluminum, and carbon). In many cases, these ancillary results are first or high-precision measurements as well. I will discuss the analysis and results of the main experiment with a focus on several of the ancillary results.