Abstract

The production of a Higgs boson in association with at least two jets receives contributions both from the fusion of weak vector bosons (VBF) and from QCD processes, especially gluon fusion (GF). The former process is important for measuring the coupling of the Higgs boson to weak bosons, whereas the latter process plays an important role in determining any CP-admixtures in the Higgs sector. In this paper we go beyond the current state-of-the-art for fixed order calculations of the GF process (i.e. one loop H + 2j including full quark mass effects) by including the all-order effects in leading log(ŝ/pt2), together with full quark mass and loop-propagator kinematic effects. We calculate the mass-dependent components and implement the resummation within the framework of High Energy Jets.The high-energy effects suppress the prediction compared to fixed order at large Δy12 and mjj (and therefore within the usual VBF cuts of widely separated jets), just as found in the limit of mt → ∞. The mass dependence is more significant than at fixed order, because the systematic inclusion of the leading logarithms in ŝ/pt2 results in a hardening of the transverse momentum of the Higgs boson, which in turn probes in more detail the loop-structure of the coupling. In particular, the full mass dependence reduces the cross section within VBF cuts by 11% compared to a calculation based just on the infinite top mass limit, but the impact of the bottom quark remains small. This all implies that the gluon-fusion contribution within VBF-cuts is less severe than current estimates suggest.

Highlights

  • In this paper we calculate the gluon fusion component of Higgs boson production in association with two jets supplementing the fixed order results with the leading logarithmic corrections in s/p2t to all orders in the coupling and including full quark mass effects

  • Higgs bosons are most copiously produced at the CERN LHC through heavy-quark mediated gluon fusion (GF), where the Born-level process is at oneloop and at order αs2

  • This section describes the matching of results within High Energy Jets (HEJ) both to the full leading-order finite quark-mass matrix elements and to the NLO cross sections obtained for infinite top mass

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Summary

Introduction

In this paper we calculate the gluon fusion component of Higgs boson production in association with two jets supplementing the fixed order results with the leading logarithmic corrections in s/p2t to all orders in the coupling and including full quark mass effects. For H + j-production at NLO, the effect of the full dependence on the heavy-quark propagator momentum is a 9% increase in the overall cross section over the result obtained in the infinite top-mass limit. In the current paper we present a calculation of higher-order perturbative corrections to the GF component of H + 2jproduction, maintaining the full dependence on the heavy-quark propagator in the heavyquark mediated coupling to the Higgs boson, and including the effects of propagating both bottom and top quarks.

Quark mass effects in Higgs boson production with HEJ
Central Higgs-boson emission
Peripheral Higgs-boson emission
The first set of next-to-leading logarithmic corrections
HEJ resummation
Real emissions
Virtual corrections
Organisation of cancellation of poles
Matching to fixed order
Matching of exclusive amplitudes
Two-jet matching with finite quark mass
Matching of leading-order results to NLO in the infinite quark mass limit
Results of finite quark masses and all-order resummation
Effects of higher perturbative orders
Effects of the finite top mass
Final results for HEJ
Conclusions
A Form factors for the Higgs-boson coupling to gluons
B Effective current for peripheral emission
Findings
C The current for a single unordered gluon emission
Full Text
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