Abstract

We present results for the Higgsstrahlung process within the GENEVA Monte Carlo framework. We combine the fully differential NNLO calculation with the higher-order resummation in the 0-jettiness resolution variable (beam-thrust). The resulting parton-level events are further showered and hadronised by Pythia8. The beam-thrust resummation is carried out to NNLL$'$ accuracy, which consistently incorporates all singular virtual and real NNLO corrections. It thus provides a natural perturbative connection between the NNLO calculation and the parton shower regime, including a systematic assessment of perturbative uncertainties. In this way, observables which are inclusive over the additional radiation are correct to NNLO, while the description of 0-jet-like resummation variables is improved beyond the parton shower approximation. We provide predictions for the 13 TeV LHC.

Highlights

  • The study of the properties of the Higgs boson forms an important part of the experimental programme at the LHC

  • Though first observed in final states with two photons, the dominant decay mode of the Higgs boson is to a pair of bottom quarks which has only recently been measured in associated production with a vector boson [1,2]

  • We present results for the Higgsstrahlung processes pp → ZH → lþl−H and pp → WÆH → lÆνlH at next-to-next-to-leading order (NNLO) matched to the PYTHIA8 parton shower according to the GENEVA method [23,28,29,30], assuming an on-shell Higgs boson

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Summary

INTRODUCTION

Though first observed in final states with two photons, the dominant decay mode of the Higgs boson is to a pair of bottom quarks which has only recently been measured in associated production with a vector boson [1,2] This class of Higgsstrahlung processes is, an interesting subject of study. In the case of ZH production, the gluon-initiated channel in which the Higgs boson couples to a top-quark loop becomes accessible beginning at Oðα2s Þ This provides a finite contribution to the next-to-next-to-leading order (NNLO) cross section and is sensitive to the presence of new physics. We present results for the Higgsstrahlung processes pp → ZH → lþl−H and pp → WÆH → lÆνlH at NNLO matched to the PYTHIA8 parton shower according to the GENEVA method [23,28,29,30], assuming an on-shell Higgs boson.

THEORETICAL FRAMEWORK
General setup
Choice of the jet resolution variables
The T 0 spectrum at NNLL0 from SCET
Scale choices and profile scales
Power-suppressed corrections to the nonsingular cumulant
NLO1 calculation and phase space mapping
Interface to the parton shower
VALIDATION
RESULTS
CONCLUSIONS
Full Text
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