A modified cluster-hadronisation model
By J. Winter, F. Krauss, G. Soff. 2003
187 citations recorded by the source corpus.
Abstract.A new phenomenological cluster-hadronisation model is presented. Its specific features are the incorporation of soft colour reconnection, a more general treatment of diquarks including their spin and giving rise to clusters with baryonic quantum numbers, and a dynamic separation of the regimes of clusters and hadrons according to their masses and flavours. The distinction between the two regions automatically leads to different cluster decay and transformation modes. Additionally, these aspects require an extension of individual cluster-decay channels that were available in previous versions of such models.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/95d36aae249c494f8fae0d766473a7bf3a2d9b28
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In Nuclear and High Energy Physics
- M. Schönherr
- F. Siegert
- S. Höche
- F. Krauss
- Steffen Schumann
- Atlas Collaboration
- Enrico Bothmann
- Stefan Hoeche
Citations in the corpus
- NLO QCD matrix elements + parton showers in e+e− → hadrons (2012, methodology): “(3.1) in SHERPA.”
- QCD matrix elements and truncated showers (2009, methodology): “Hadron-level results are produced using SHERPA with the fragmentation module AHADIC++ [58], the hadron and τ decay package HADRONS++ [59] and a simulation of extra QED radiation through PHOTONS++ [60].”
- Event generation with Sherpa 2.2 (2019, methodology): “There are currently two successful approaches included in event generators to describe the transition from the quanta of perturbative QCD, the quarks and gluons, to the observable hadrons, namely the Lund string model [33, 168] used in PYTHIA [34, 1] and cluster fragmentation models [169], such as t”
- Event generation with SHERPA 1.1 (2008, background): “It should be noted that AHADIC, essentially based on [ 37 ], indeed differs from the original versions, cf. Sec.”
- A critical appraisal of NLO+PS matching methods (2011, methodology): “The predictions presented here include simulation of hadronisation [41] and multiple parton interactions (MPI) [42] as well as hadron decays [43] and higher-order QED corrections to the h→ ττ decay [44].”