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 $\mathcal{O}(\alpha_s^2)$ contributions that occur in production for these processes: those mediated by the exchange of a single off-shell vector boson in the $s$-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 $H\rightarrow b\bar{b}$, $\gamma\gamma$ and $WW^*$. The treatment of the $H\rightarrow b\bar{b}$ decay includes QCD corrections at NLO. We use the recently developed $N$-jettiness regularization procedure, and study its viability in the presence of a large final-state phase space by studying $pp\rightarrow V(H\rightarrow WW^*) \rightarrow$ leptons.

Highlights

  • Vertex at high momentum transfer while keeping the final state vector and Higgs bosons on-shell, for instance by looking in the region of large mV H

  • 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 all O(αs2) contributions that occur in production for these processes: those mediated by the exchange of a single off-shell vector boson in the s-channel, and those which arise from the coupling of the Higgs boson to a closed loop of fermions

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Summary

Introduction

Vertex at high momentum transfer while keeping the final state vector and Higgs bosons on-shell, for instance by looking in the region of large mV H. When τN < τNcut SCET [28,29,30,31,32,33] provides a factorization theorem [23, 33] that can be used to compute the cross section An advantage of this method is that it can be applied to coloured final states with jets. We will apply the recently-developed SCET formalism to a detailed phenomenological study, including the process V H → V W W →leptons Such decays have not previously been included in NNLO codes, but are studied experimentally. Given the large and intricate final state phase space (22 dimensions for the double-real part) this is a good example to test the feasibility of the SCET regularization to provide NNLO predictions for complicated phenomenological applications. Our results are implemented in MCFM [43,44,45], and are available in MCFM 8.0 [46]

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