2016
DOI: 10.1140/epjc/s10052-016-4430-0
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Reweighting QCD matrix-element and parton-shower calculations

Abstract: We present the implementation and validation of the techniques used to efficiently evaluate parametric and perturbative theoretical uncertainties in matrix-element plus parton-shower simulations within the Sherpa eventgenerator framework. By tracing the full α s and PDF dependences, including the parton-shower component, as well as the fixed-order scale uncertainties, we compute variational event weights on-the-fly, thereby greatly reducing the computational costs to obtain theoretical-uncertainty estimates.

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Cited by 94 publications
(87 citation statements)
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“…Finally, we want to emphasize that despite the uncertainties currently present in partonshower generators [137][138][139][140], parton showers in particular (and QCD resummation techniques more generally) will be essential for understanding quark/gluon discrimination. Fixed-order QCD calculations cannot reliably probe the very soft and very collinear structure of jets, which is precisely where valuable information about quark/gluon radiation patterns reside.…”
Section: Jhep07(2017)091mentioning
confidence: 99%
“…Finally, we want to emphasize that despite the uncertainties currently present in partonshower generators [137][138][139][140], parton showers in particular (and QCD resummation techniques more generally) will be essential for understanding quark/gluon discrimination. Fixed-order QCD calculations cannot reliably probe the very soft and very collinear structure of jets, which is precisely where valuable information about quark/gluon radiation patterns reside.…”
Section: Jhep07(2017)091mentioning
confidence: 99%
“…The dijet system with the cutp ⊥ ≥ 500 GeV as underlying hard process is typically accompanied by a large number of additional jets. Given the nature of the reweighting algorithm of [22] (and similarly for [23,44]) this may easily result in fluctuating weights. In addition we expect larger fluctuations in the nonsingular-term variations for the helicity shower, compared to the helicity-independent one.…”
Section: Example Applicationmentioning
confidence: 99%
“…[31] or MadGraph [32]. Let us explain what the advantages and disadvantages are behind such a choice.…”
Section: On Reliability Of the Tauspinner Re-weighting Approachmentioning
confidence: 99%