Abstract

In this paper we present a Next-to-Next-to Leading Order (NNLO) calculation of the production of a Higgs boson in association with a massive vector boson. We include the decays of the unstable Higgs and vector bosons, resulting in a fully flexible parton-level Monte Carlo implementation. We also include all O(αs2)\mathcal{O}(α_s^2) contributions that occur in production for these processes: those mediated by the exchange of a single off-shell vector boson in the ss-channel, and those which arise from the coupling of the Higgs boson to a closed loop of fermions. We study final states of interest for Run II phenomenology, namely H→bbˉH\rightarrow b\bar{b}, γγγγ and WW∗WW^*. The treatment of the H→bbˉH\rightarrow b\bar{b} decay includes QCD corrections at NLO. We use the recently developed NN-jettiness regularization procedure, and study its viability in the presence of a large final-state phase space by studying pp→V(H→WW∗)→pp\rightarrow V(H\rightarrow WW^*) \rightarrow leptons.

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