In its first running period, the LHC has produced more W bosons than any accelerator before. This makes the LHC experiments hotbeds of electroweak physics. Although the ultimate precision in the measurement of electroweak parameters in many cases is still held by LEP, SLC or the Tevatron, the LHC has opened new views on measurements at high scales, especially in the field of multi-boson couplings. Furthermore, at the LHC the electroweak gauge bosons are used in a wide range of measurements that constrain the parton densities of the proton in ways that are complementary to previous results. The future promises further exciting results, among them W -boson mass measurements with unprecedented precision and the detailed study of vector-boson scattering.
IntroductionPrecision measurements of electroweak (EW) parameters at the LHC are commonly limited in precision by the high pile-up and by the more complicated initial state compared to lepton colliders. Nevertheless, measurements of EW parameters are still of interest, especially for parameters that have a scale dependence because the high centre-of-mass energy of the LHC allows for studying previously inaccessible values of the scale. The measurements will typically have considerable uncertainties due to the underlying proton parton distribution functions (PDFs) and to other aspects of M. Boonekamp (B) CEA, IRFU,