2010
DOI: 10.1007/jhep08(2010)098
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Supersymmetric top and bottom squark production at hadron colliders

Abstract: The scalar partners of top and bottom quarks are expected to be the lightest squarks in supersymmetric theories, with potentially large cross sections at hadron colliders. We present predictions for the production of top and bottom squarks at the Tevatron and the LHC, including next-to-leading order corrections in supersymmetric QCD and the resummation of soft gluon emission at next-to-leading-logarithmic accuracy. We discuss the impact of the higher-order corrections on total cross sections and transverse-mom… Show more

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Cited by 240 publications
(267 citation statements)
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“…The SUSY signal samples were produced at leading order using MadGraph5 [50,164,165] with a CTEQ6L1 PDF, with the cross section rescaled using a K-factor calculated with next-to-leading order (NLO) supersymmetric QCD corrections and the resummation of soft gluon emission at next-to-leading-logarithmic (NLL) accuracy using the NLL-fast computer program [166][167][168]. In view of the fact that for large ∆m, the veto of any event with a fourth jet with p T > 30…”
Section: Discussionmentioning
confidence: 99%
“…The SUSY signal samples were produced at leading order using MadGraph5 [50,164,165] with a CTEQ6L1 PDF, with the cross section rescaled using a K-factor calculated with next-to-leading order (NLO) supersymmetric QCD corrections and the resummation of soft gluon emission at next-to-leading-logarithmic (NLL) accuracy using the NLL-fast computer program [166][167][168]. In view of the fact that for large ∆m, the veto of any event with a fourth jet with p T > 30…”
Section: Discussionmentioning
confidence: 99%
“…In all cases, the mass of the top quark is fixed at 172.5 GeV. Signal cross-sections are calculated to NLO in the strong coupling constant, adding the resummation of soft-gluon emission at next-to-leading-logarithmic accuracy (NLO+NLL) [45,65,66]. The nominal cross-section and the uncertainty are based on predictions using different PDF sets and factorisation and renormalisation scales, as described in ref.…”
Section: Jhep08(2017)006mentioning
confidence: 99%
“…We also consider the case where a jet is replaced by heavy flavor quark. In each figure we show the current limit on the pair-production cross section times BR 2 , normalized to the NLO+NLL cross section of a scalar colored triplet taken from [20][21][22]. Presented this way, when a single mode dominates the decay (namely BR = 1), the y axis corresponds to the number of copies of the X representation that are experimentally allowed.…”
Section: Jhep02(2017)104mentioning
confidence: 99%