Abstract:We present a Monte Carlo generator that implements significant theoretical improvements in the simulation of top-quark pair production and decay at the LHC. Spin correlations and off-shell effects in top-decay chains are described in terms of exact matrix elements for pp → + ν l −ν l bb at order α 4 α 2 S plus full NLO QCD corrections, where the leptons and l belong to different families, and b quarks are massive. Thus, the contributions from tt and W t single-top production, plus contributions without top res… Show more
The next-to-leading order QCD corrections to the top-bottom interference contribution to H + j production at the LHC are presented. The QCD corrections to the interference are large and similar to the QCD corrections to the top-mediated Higgs production cross section. There is also a significant reduction in the mass-renormalization scheme uncertainty once the NLO QCD prediction for the interference is employed.13th International Symposium on Radiative Corrections
The next-to-leading order QCD corrections to the top-bottom interference contribution to H + j production at the LHC are presented. The QCD corrections to the interference are large and similar to the QCD corrections to the top-mediated Higgs production cross section. There is also a significant reduction in the mass-renormalization scheme uncertainty once the NLO QCD prediction for the interference is employed.13th International Symposium on Radiative Corrections
“…[78] and [79,80] resonance aware matching has been proposed within the MC@NLO and Powheg frameworks respectively, with focus on narrow coloured resonances. In our configuration the resonances are broader and the interference plays a more important role.…”
Scalar and pseudo-scalar resonances decaying to top quarks are common predictions in several scenarios beyond the standard model (SM) and are extensively searched for by LHC experiments. Challenges on the experimental side require optimising the strategy based on accurate predictions. Firstly, QCD corrections are known to be large both for the SM QCD background and for the pure signal scalar production. Secondly, leading order and approximate next-to-leading order (NLO) calculations indicate that the interference between signal and background is large and drastically changes the lineshape of the signal, from a simple peak to a peak-dip structure. Therefore, a robust prediction of this interference at NLO accuracy in QCD is necessary to ensure that higher-order corrections do not alter the lineshapes. We compute the exact NLO corrections, assuming a point-like coupling between the scalar and the gluons and consistently embedding the calculation in an effective field theory within an automated framework, and present results for a representative set of beyond the SM benchmarks. The results can be further matched to parton shower simulation, providing more realistic predictions. We find that NLO corrections are important and lead to a significant reduction of the uncertainties. We also discuss how our computation can be used to improve the predictions for physics scenarios where the gluon-scalar loop is resolved and the effective approach is less applicable.
“…[35], the process pp → bb4f has been matched consistently to parton showers, as presented recently in ref. [36]. For hadron colliders, corresponding NLO QCD corrections to top-quark pair production in association with a Higgs boson [37] or a jet [38,39] including leptonic decays have also been studied.…”
Section: Jhep12(2016)075mentioning
confidence: 99%
“…Finally we want to note, that the resonance-aware FKS subtraction scheme, including a definite resonance history assignment in the event output, enables a consistent matching of fixed-order NLO predictions with parton shower generators for processes with intermediate resonances [35,36]. To this end, all relevant resonance histories should be taken into account.…”
We present predictions for tt and ttH production and decay at future lepton colliders including non-resonant and interference contributions up to next-to-leading order (NLO) in perturbative QCD. The obtained precision predictions are necessary for a future precise determination of the top-quark Yukawa coupling, and allow for top-quark phenomenology in the continuum at an unprecedented level of accuracy. Simulations are performed with the automated NLO Monte-Carlo framework Whizard interfaced to the OpenLoops matrix element generator.
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