2006
DOI: 10.1140/epjc/s2006-02552-4
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Infrared-safe definition of jet flavour

Abstract: It is common, in both theoretical and experimental studies, to separately discuss quark and gluon jets. However, even at parton level, widely-used jet algorithms fail to provide an infrared safe way of making this distinction. We examine the origin of the problem, and propose a solution in terms of a new 'flavour-k t ' algorithm. As well as being of conceptual interest this can be a powerful tool when combining fixed-order calculations with multi-jet resummations and parton showers. It also has applications to… Show more

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Cited by 181 publications
(232 citation statements)
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References 35 publications
(58 reference statements)
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“…This is the strategy adopted in ref. [56]. While this definition neglects the impact of hadronization, it does allow for the calculation of quark jet cross sections at all perturbative orders, including quantum corrections.…”
Section: Jhep07(2017)091mentioning
confidence: 99%
“…This is the strategy adopted in ref. [56]. While this definition neglects the impact of hadronization, it does allow for the calculation of quark jet cross sections at all perturbative orders, including quantum corrections.…”
Section: Jhep07(2017)091mentioning
confidence: 99%
“…An algorithm for doing so was proposed by Banfi, Salam, and Zanderighi in [20]. Their idea was to count the number of quarks minus anti-quarks in a jet.…”
Section: Theoretical Considerationsmentioning
confidence: 99%
“…This is because the requirement v ≪ 1 forces all radiation to be either soft or collinear. At perturbative level it is also possible to unambiguously attribute a partonic subprocess to the event, for example qq → qq (doing so requires a flavour infrared and collinear safe procedure, as in [72], but the result is JHEP06(2010)038 independent of the choice of the procedure). Here we will use B to label the event's 2 → 2 kinematics and δ to label its 2 → 2 flavour structure.…”
Section: Nll Resummation Structurementioning
confidence: 99%
“…We therefore extended it so as to have access to the flavour of both incoming and outgoing partons in the calculation of σ 0 , σ 1 and Σ 1 (v), though not forΣ 2 (v) since its colour-channel separation is not needed for NNLL Σ accuracy. To assign events with more than two outgoing partons to a definite 2 → 2 colour channel we used the exclusive flavour-k t algorithm of [72] to cluster events to a 2 → 2 topology while keeping track of flavour in an infrared safe manner. During the clustering procedure, quarks of different flavour might end up in the same jet, giving rise to multi-flavoured jets, i.e.…”
Section: Jhep06(2010)038mentioning
confidence: 99%