We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoton-plus-jet production at the LHC. We compute fully differential distributions by combining two-loop virtual corrections with one-loop real radiation using antenna subtraction to cancel infrared divergences. We observe significant corrections at NLO which demonstrate the importance of combining these corrections with the quark-induced diphoton-plus-jet channel at next-to-next-to-leading order (NNLO)
The production of jets in charged current deep inelastic scattering (CC DIS) constitutes a class of ...
We report the first calculation of fully differential jet production at leading color in all partoni...
We study the resummation of soft gluon emission corrections to the production of a top-antitop pair ...
We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoto...
We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoto...
We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoto...
We report the calculation of next-to-next-to-leading order QCD corrections in the purely gluonic cha...
In this paper we present a next-to-next-to-leading order (NNLO) calculation of the process pp → γγ t...
We present the virtual QCD corrections to gluon–gluon scattering due to the interference of tree- a...
Abstract: We calculate the NNLO QCD corrections to diphoton production with an additional jet at the...
We compute the cross section and differential distributions for the production of a Z boson in asso...
To match the increasing precision of modern collider experiments, theory must aim to achieve percent...
To match the increasing precision of modern collider experiments, theory must aim to achieve percent...
In this thesis, we present recent advances at the precision frontier of higher-order quantum chromod...
We compute the next-to-leading order (NLO) QCD corrections to the gg→W+W−→l1+ν1l2−ν¯2 process, media...
The production of jets in charged current deep inelastic scattering (CC DIS) constitutes a class of ...
We report the first calculation of fully differential jet production at leading color in all partoni...
We study the resummation of soft gluon emission corrections to the production of a top-antitop pair ...
We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoto...
We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoto...
We compute the next-to-leading order (NLO) QCD corrections to the gluon-fusion subprocess of diphoto...
We report the calculation of next-to-next-to-leading order QCD corrections in the purely gluonic cha...
In this paper we present a next-to-next-to-leading order (NNLO) calculation of the process pp → γγ t...
We present the virtual QCD corrections to gluon–gluon scattering due to the interference of tree- a...
Abstract: We calculate the NNLO QCD corrections to diphoton production with an additional jet at the...
We compute the cross section and differential distributions for the production of a Z boson in asso...
To match the increasing precision of modern collider experiments, theory must aim to achieve percent...
To match the increasing precision of modern collider experiments, theory must aim to achieve percent...
In this thesis, we present recent advances at the precision frontier of higher-order quantum chromod...
We compute the next-to-leading order (NLO) QCD corrections to the gg→W+W−→l1+ν1l2−ν¯2 process, media...
The production of jets in charged current deep inelastic scattering (CC DIS) constitutes a class of ...
We report the first calculation of fully differential jet production at leading color in all partoni...
We study the resummation of soft gluon emission corrections to the production of a top-antitop pair ...