Hadronic ZZ, ${\mathit{W}}^{\mathrm{-}}$${\mathit{W}}^{+}$, and ${\mathit{W}}^{\pm }$Z production with QCD corrections and leptonic decays

The processes ${\mathit{pp}}^{\left(\mathrm{-}\right)}$→${\mathit{V}}_1$ ${\mathit{V}}_2$+X→${\mathit{l}}_1$l${\mathrm{¯}}_1$ ${\mathit{l}}_2$l${\mathrm{¯}}_2$+X, where ${\mathit{V}}_{\mathit{i}}$=${\mathit{W}}^{\pm }$ or Z and ${\mathit{l}}_{\mathit{i}}$ denotes a lepton, are calculated to O(${\mathrm{\alpha }}_{\mathit{s}}$). Total and differential cross sections, with acceptance cuts imposed on the final state leptons, are given for the Fermilab Tevatron and CERN LHC center of mass energies. Inclusive and exclusive 0-jet and 1-jet cross sections are given. The transverse momenta spectra of the leptons are significantly enhanced at high ${\mathit{p}}_{\mathit{T}}$ by the QCD radiative corrections, especially at the LHC energy. Invariant mass and angular distributions are scaled up in magnitude by the QCD radiative corrections, but are little changed in shape.