Precision study of W−W+HW^-W^+H production including parton shower effects at the CERN Large Hadron Collider

preprint2019arXivOpen access

Abstract

The precision study of W−W+HW^-W^+H production with subsequent W±→l±νl(−)W^{\pm} \rightarrow l^{\pm} \overset{ _{(-)}}{ν_{l}} and H→bbˉH \rightarrow b\bar{b} decays at the LHC can help us to study the Higgs gauge couplings and to search for new physics beyond the SM. In this paper, we calculate the shower-matched NLO QCD correction and the EW corrections from the qqˉq\bar{q} annihilation and photon-induced channels to the W−W+HW^-W^+H production at the 14 TeV14~ {\rm TeV} LHC, and deal with the subsequent decays of Higgs and W±W^{\pm} bosons by adopting the {\sc MadSpin} method. Both the integrated cross section and some kinematic distributions of W±W^{\pm}, HH and their decay products are provided. We find that the QCD correction enhances the LO differential cross section significantly, while the EW correction from the qqˉq\bar{q} annihilation channel obviously suppresses the LO differential cross section, especially in the high energy phase-space region due to the Sudakov effect. The qγqγ- and γγγγ-induced relative corrections are positive, and insensitive to the transverse momenta of W±W^{\pm}, HH and their decay products. These photon-induced corrections compensate the negative qqˉq\bar{q}-initiated EW correction, and become the dominant EW contribution as the increment of the pppp colliding energy. The parton shower (PS) effects on the kinematic distributions are nonnegligible. The PS relative correction to the bb-jet transverse momentum distribution can exceed 100%100\% in the high pT,bp_{T, b} region. We also investigate the scale and PDF uncertainties, and find that the theoretical error of the QCD+EW+qγ+γγ{\rm QCD}+{\rm EW}+qγ+γγ corrected integrated cross section mainly comes from the renormalization scale dependence of the QCD correction.

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