effects of pileup (additional interactions from the same or nearby bunch crossings) and are weighted to reproduce the distribution of the number of interactions in data.

The signal samples are simulated with $\MGvATNLO$ v2.2.2 [@Alwall:2014hca] at next-to-leading order (NLO) in perturbative QCD with FxFx merging [@Frederix:2012ps] for the $\Pg\Pg\PH$, VBF, V, and [$\ttbar\PH$]{}production processes. These samples include production of up to two additional jets in association with the Higgs boson. The parton-level samples are interfaced to $\PYTHIA 8.205$ [@Sjostrand:2014zea] with the CUETP8M1 [@CUETP8M1] underlying event tune, for parton showering, underlying event modeling, and hadronization. In order to match the prediction for $\Pg\Pg\PH$ production mechanism from the [<span style="font-variant:small-caps;">nnlops</span>]{} program [@Hamilton:2013fea; @PowhegMinlo; @Kardos:2014dua], the generated events are weighted according to the Higgs boson and the number of jets in the event. The [<span style="font-variant:small-caps;">nnlops</span>]{} program has the advantage of predicting at next-to-next-to-leading-order (NNLO) accuracy, both the differential cross section with respect to the QCD radiative effects and the normalization of the inclusive cross section. The $\Pg\Pg\PH$ samples are also generated with the v2 program [@powheg1; @powheg2; @powheg3; @powheg-ggH; @Bagnaschi2012], which includes production of one additional jet, in order to provide an alternative theoretical prediction for inclusive measurements and measurements involving the 