2022
DOI: 10.48550/arxiv.2203.06799
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Future prospects for parton showers

Abstract: In this brief Snowmass White Paper for the Theory Frontier, we argue that there have been important recent developments in the algorithms used to generate a simulated parton shower and that further progress can be achieved in the coming decade. A much more detailed exposition can be found in a corresponding White Paper of the Energy Frontier. * Herwig, however rearranges the ordering of splittings in its default parton shower so that larger angle splittings come first.

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“…In this case, our NLO predictions are generated with or without the inclusion of real and virtual EW corrections, allowing us to investigate different settings in the evaluation of EW-sensitive events in Herwig 7. The predicted signals are compared with the experimental measurements from the ATLAS collaboration [27,28] and against third-party theoretical predictions within the k t -factorisation framework [29][30][31], using the unintegrated parton distribution functions (UPDFs) of Kimber-Martin-Ryskin (KMR) [32,33]. The latter framework has been used as a control signal since its validity in accurately predicting the behaviour of experimental observations has been repeatedly proven to be independent of the use parton shower enhancements [34][35][36][37][38][39], while being computationally expensive and unsuitable for use in general-purpose event generators [45][46][47][48]. Note that the production of W ± and Z 0 bosons in association with hadronic jets have been studied extensively in the literature, e.g.…”
Section: Introductionmentioning
confidence: 99%
“…In this case, our NLO predictions are generated with or without the inclusion of real and virtual EW corrections, allowing us to investigate different settings in the evaluation of EW-sensitive events in Herwig 7. The predicted signals are compared with the experimental measurements from the ATLAS collaboration [27,28] and against third-party theoretical predictions within the k t -factorisation framework [29][30][31], using the unintegrated parton distribution functions (UPDFs) of Kimber-Martin-Ryskin (KMR) [32,33]. The latter framework has been used as a control signal since its validity in accurately predicting the behaviour of experimental observations has been repeatedly proven to be independent of the use parton shower enhancements [34][35][36][37][38][39], while being computationally expensive and unsuitable for use in general-purpose event generators [45][46][47][48]. Note that the production of W ± and Z 0 bosons in association with hadronic jets have been studied extensively in the literature, e.g.…”
Section: Introductionmentioning
confidence: 99%