Heavy quark radiation in NLO+PS POWHEG generators
arXiv:1711.06281 · doi:10.1140/epjc/s10052-018-5638-y
Abstract
In this paper we deal with radiation from heavy quarks in the context of next-to-leading order calculations matched to parton shower generators. A new algorithm for radiation from massive quarks is presented that has considerable advantages over the one previously employed. We implement the algorithm in the framework of the , and compare it with the previous one in the case of the generator for bottom production in hadronic collisions, and in the case of the generator for top production and decay.
14 pages, 13 figures, LaTeX
References in corpus (13)
- An Introduction to PYTHIA 8.2
- Parton distributions for the LHC
- Matching NLO QCD computations with Parton Shower simulations: the POWHEG method
- Implications of CTEQ global analysis for collider observables
- A parton shower algorithm based on Catani-Seymour dipole factorisation
- Parton Distributions for LHC
- An NLO+PS generator for and production and decay including non-resonant and interference effects
- Evidence for the decay with the ATLAS detector
- Evidence for the Higgs boson decay to a bottom quark-antiquark pair
- Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair
- NLO Antenna Subtraction with Massive Fermions
- Measurement of top quark pair differential cross-sections in the dilepton channel in collisions at = 7 and 8 TeV with ATLAS
- Measurement of the b-hadron production cross section using decays to D*muX final states in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- The subtraction method: electroweak corrections and power suppressed contributions
- Top-Yukawa contributions to bbH production at the LHC
- NLO and off-shell effects in top quark mass determinations
- High-energy QCD dynamics from bottom flavor fragmentation at the Hi-Lumi LHC
- B-hadron production at the LHC from bottom-quark pair production at NNLO+PS