The Weinberg angle or weak mixing angle is a parameter in the Weinberg–Salam theory of the electroweak interaction, part of the Standard Model of particle physics, and is usually denoted as. It is the angle by which spontaneous symmetry breakingrotates the original and B0vector boson plane, producing as a result the boson, and the photon. It also gives the relationship between the masses of the W and Z bosons, The angle can be expressed in terms of the and couplings, The electric charge is then expressible in terms of it, = = ; see the Figure. As the value of the mixing angle is currently determined empirically, it has been mathematically defined as The value of varies as a function of the momentum transfer,, at which it is measured. This variation, or 'running', is a key prediction of the electroweak theory. The most precise measurements have been carried out in electron–positron collider experiments at a value of, corresponding to the mass of the Z boson,. In practice the quantity is more frequently used. The 2004 best estimate of, at, in the scheme is, which averages over measurements made in different processes and at different detectors. Atomicparity violation experiments yield values for at smaller values of, below 0.01 GeV/c, but with much lower precision. In 2005 results were published from a study of parity violation in Møller scattering in which a value of was obtained at, establishing experimentally the 'running' of the weak mixing angle. These values correspond to a Weinberg angle of ~30°. LHCb measured in 7 and 8 TeV proton-proton collisions an effective angle of = 0.23142, though the value of for this measurement is determined by the partonic collision energy, which is close to the Z boson mass. CODATA 2018 gives the value Note, however, that the specific value of the angle is not a prediction of the standard model: it is an open, unfixed parameter. However, it is constrained and predicted through other measurements of Standard Model quantities. At this time, there is no generally accepted theory that explains why the measured value is what it is.
