Abstract

We consider the production of a Higgs boson in association with two electroweak vector bosons at hadron colliders. In particular, we examine $\gamma\gamma H$, $\gamma ZH$, $ZZH$, and $W^{+}W^{-}H$ production at the LHC (14 TeV), HE-LHC (27 TeV), and FCC-hh (100 TeV) colliders. Our main focus is to estimate the gluon-gluon ($gg$) channel ($gg \to VV^\prime H$) contributions to $pp \to VV^\prime H~(V,V^\prime=\gamma,Z,W)$ and compare them with corresponding contributions arising from the quark-quark ($qq$) channel. Technically, the leading order $gg$ channel contribution to $pp \to VV^\prime H$ cross section is an NNLO correction in $\alpha_s$. In the processes under consideration, we find that in the $gg$ channel, $W^{+}W^{-}H$ has the largest cross section. However, relative contribution of the $gg$ channel is more important for the $pp \to ZZH$ production. At the FCC-hh, $gg \to ZZH$ contribution is comparable with the NLO QCD correction to $qq \to ZZH$. We also compute the cross sections when $W$ and $Z$-bosons are polarized. In the production of $W^{+}W^{-}H$ and $ZZH$, we find that the $gg$ channel contributes more significantly when the vector bosons are longitudinally polarized. By examining such events, one can increase the fraction of the $gg$ channel contribution to these processes. Further, we have studied beyond-the-standard-model effects in the $\kappa$-framework. We find that the $gg$ channel processes $ZZH$ and $WWH$ have very mild dependence on $\kappa_\lambda$, but strong dependence on $\kappa_t$ and $\kappa_V$. The $qq$ channel processes mainly depend on $\kappa_V$. Dependence of the $gg$ channel contribution on $\kappa_V$ is stronger than that of the $qq$ channel contribution. Therefore focusing on events with longitudinally polarized $W$ and $Z$-bosons, one can find stronger dependence on $\kappa_V$ that can help us measure this parameter.

Highlights

  • After the discovery of a Higgs-like resonance, with a mass of 125 GeV, at the Large Hadron Collider (LHC) in 2012, various properties of this new particle have been studied

  • Couplings of this new particle with the fermions and gauge bosons predicted in the standard model (SM) are getting constrained as more and more data are being analyzed by the LHC experiments [2,3,4]

  • Since loop-induced processes are sensitive to new physics, we study the effect of new physics in all VVH processes using a common beyond the standard model (BSM) framework—the κ framework

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Summary

INTRODUCTION

After the discovery of a Higgs-like resonance, with a mass of 125 GeV, at the Large Hadron Collider (LHC) in 2012, various properties of this new particle have been studied. The spin and parity measurements have established it as a 0þ state at 99.9% CL against alternative scenarios [1] Couplings of this new particle with the fermions and gauge bosons predicted in the standard model (SM) are getting constrained as more and more data are being analyzed by the LHC experiments [2,3,4]. Because of many electroweak couplings involved and the loop-induced nature of gg → VVH processes, their cross sections are expected to be small They can be important at high energy hadron colliders like the 100 TeV pp collider such as the proposed hadronic Future Circular Collider (FCC-hh) facility at CERN [42] and the Super Proton-Proton Collider (SPPC) facility in China [43].

GLUON FUSION CONTRIBUTION TO VVH
BSM PARAMETRIZATION
CALCULATION AND CHECKS
NUMERICAL RESULTS
Remarks on anomalous HHH and HHVV couplings
CONCLUSIONS
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