Physics at a 100 TeV pp collider: Higgs and EW symmetry breaking studies
(2016)
Fully Differential Vector-Boson-Fusion Higgs Production at Next-to-Next-to-Leading Order.
Physical review letters 115:8 (2015) 082002
Abstract:
We calculate the fully differential next-to-next-to-leading-order (NNLO) corrections to vector-boson fusion (VBF) Higgs boson production at proton colliders, in the limit in which there is no cross talk between the hadronic systems associated with the two protons. We achieve this using a new "projection-to-Born" method that combines an inclusive NNLO calculation in the structure-function approach and a suitably factorized next-to-leading-order VBF Higgs plus three-jet calculation, using appropriate Higgs plus two-parton counterevents. An earlier calculation of the fully inclusive cross section had found small NNLO corrections, at the 1% level. In contrast, the cross section after typical experimental VBF cuts receives NNLO contributions of about (5-6)%, while differential distributions show corrections of up to (10-12)% for some standard observables. The corrections are often outside the next-to-leading-order scale-uncertainty band.NNLOPS accurate Drell-Yan production
Journal of High Energy Physics Springer Nature 2014:9 (2014) 134
Electroweak ZZjj production in the Standard Model and beyond in the POWHEG-BOX V2
Journal of High Energy Physics 2014:3 (2014)
Abstract:
We present an implementation of electroweak ZZjj production in the POWHEG BOX V2 framework, an upgrade of the POWHEG BOX program which includes a number of new features that are particularly helpful for high-multiplicity processes. We consider leptonic and semi-leptonic decay modes of the Z bosons, and take non-resonant contributions and spin correlations of the final-state particles into account. In the case of decays to leptons, we also include interactions beyond the Standard Model that arise from an effective Lagrangian which includes CP conserving and violating operators up to dimension six. We find that while leptonic distributions are very sensitive to anomalous couplings, because of the small cross-section involved, these analyses are feasible only after a high-luminosity upgrade of the LHC. We consider the cases of a 14 TeV, 33 TeV and 100 TeV machine and discuss the limits that can be placed on those couplings for different luminosities. Open Access, © The Authors. Article funded by SCOAP3.Feynman Rules for QCD in Space-Cone Gauge
ArXiv 1201.1441 (2012)