We present the results of a comprehensive study of W and Z production in high-energy ep
collisions. The processes ep→ eW±X, ep→ νWsu− X, ep→ eZX and ep→ νZX are …

The purely electroweak (EW) cross section for the production of two jets in association with a
Z boson, in proton–proton collisions at\(\sqrt {s}= 8\,\text {TeV}\), is measured using data …

Electroweak measurements performed with data taken at the electron–positron collider LEP
at CERN from 1995 to 2000 are reported. The combined data set considered in this report …

We present exact tree level matrix elements for all the single weak boson production
processes to order e 3 in very high energy e+ e− collisions; e+ e−→ e±v (−) c W∓, e+ e− Z …

To match the precision of present and future measurements of W-boson production at
hadron colliders electroweak radiative corrections must be included in the theory …

A search for excited electrons is performed using the full e±p data sample collected by the
H1 experiment at HERA, corresponding to a total luminosity of 475 pb− 1. The electroweak …

This note presents a combination of published and preliminary electroweak results from the
four LEP collaborations ALEPH, DELPHI, L3 and OPAL based on electron-positron collision …

Higgs-strahlung e+ e−→ ZH and WW fusion e+ e−→ ν eν eH are the most important
mechanisms for the production of Higgs bosons in e+ e− collisions at LEP2 and future e+ e …

The production of electrons with very high transverse momentum has been studied in the
UA2 experiment at the CERN ̄ pp collider (\sqrt s= 540 GeV). From a sample of events …

The mass of the W boson is determined from the direct reconstruction of W decays in WW→
qq̄qq̄ and WW→ ℓνqq̄ events in e+ e-collisions at LEP. The data sample corresponds to …