We present the calculation of the next-to-leading order QCD corrections to electroweak p p -> e+ nu_e mu+ mu- jj and p p -> e- nubar_e mu+ mu- jj production at the CERN LHC in the form of a fully flexible parton-level Monte Carlo program. The QCD corrections to the total cross sections are modest, changing the leading-order results by less than 10%. At the Born level, the shape of kinematic distributions can depend significantly on the choice of factorization scale. This theoretical uncertainty is strongly reduced by the inclusion of the next-to-leading order QCD corrections
Radiative corrections of strong and electroweak interactions are presented at next-to-leading order ...
We present the full next-to-leading-order electroweak and QCD corrections to vector-boson scattering...
We compute the next-to-leading order QCD corrections to WZ+jet production at the Tevatron and the LH...
We present the calculation of the next-to-leading-order QCD corrections to electroweak pp -> e(+)...
Vector-boson fusion processes are an important tool for the study of electroweak symmetry breaking a...
We present a next-to-leading-order QCD calculation for e+\nu e\mu+\nu\mu jj production in vector-bos...
The computation of the O(alpha(s)) QCD corrections to the cross sections for W+W-gamma and ZZ gamma ...
We present a calculation of next-to-leading order QCD corrections to QCD-induced ZZ production in as...
The production of W or Z bosons in association with two jets is an important background to the Higgs...
AbstractSlepton pairs can be produced in vector–boson fusion processes at hadron colliders. The next...
NLO-QCD corrections to vector boson pair production via weak boson fusion have recently been calcula...
AbstractWe compute the next-to-leading order (NLO) QCD corrections to the gg→W+W−→l1+ν1l2−ν¯2 proces...
Slepton pairs can be produced in vector-boson fusion processes at hadron colliders. The next-to-lead...
AbstractWe present a calculation of the full next-to-leading order QCD corrections to the scattering...
We have studied the effect of one-loop logarithmic electroweak radiative corrections on WZ and $W\ga...
Radiative corrections of strong and electroweak interactions are presented at next-to-leading order ...
We present the full next-to-leading-order electroweak and QCD corrections to vector-boson scattering...
We compute the next-to-leading order QCD corrections to WZ+jet production at the Tevatron and the LH...
We present the calculation of the next-to-leading-order QCD corrections to electroweak pp -> e(+)...
Vector-boson fusion processes are an important tool for the study of electroweak symmetry breaking a...
We present a next-to-leading-order QCD calculation for e+\nu e\mu+\nu\mu jj production in vector-bos...
The computation of the O(alpha(s)) QCD corrections to the cross sections for W+W-gamma and ZZ gamma ...
We present a calculation of next-to-leading order QCD corrections to QCD-induced ZZ production in as...
The production of W or Z bosons in association with two jets is an important background to the Higgs...
AbstractSlepton pairs can be produced in vector–boson fusion processes at hadron colliders. The next...
NLO-QCD corrections to vector boson pair production via weak boson fusion have recently been calcula...
AbstractWe compute the next-to-leading order (NLO) QCD corrections to the gg→W+W−→l1+ν1l2−ν¯2 proces...
Slepton pairs can be produced in vector-boson fusion processes at hadron colliders. The next-to-lead...
AbstractWe present a calculation of the full next-to-leading order QCD corrections to the scattering...
We have studied the effect of one-loop logarithmic electroweak radiative corrections on WZ and $W\ga...
Radiative corrections of strong and electroweak interactions are presented at next-to-leading order ...
We present the full next-to-leading-order electroweak and QCD corrections to vector-boson scattering...
We compute the next-to-leading order QCD corrections to WZ+jet production at the Tevatron and the LH...