2009
DOI: 10.1103/physrevlett.102.111802
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Threshold Resummation for Squark-Antisquark and Gluino-Pair Production at the LHC

Abstract: We study the effect of soft gluon emission in the hadroproduction of squark-antisquark and gluino-gluino pairs at the next-to-leading logarithmic (NLL) accuracy within the framework of the minimal supersymmetric model. The one-loop soft anomalous dimension matrices controlling the colour evolution of the underlying hard-scattering processes are calculated. We present the resummed total cross sections and show numerical results for proton-proton collisions at 14 TeV.The size of the NLL contribution to the cross… Show more

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Cited by 353 publications
(399 citation statements)
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“…(2.5), (2.6) reproduce the known results for heavy quark-antiquark (squark-antisquark) pair-production soft anomalous dimension [32,33,[38][39][40] in the limit p B → 0. Also, our result for Γ qq→klB agrees with the result obtained in the SCET framework in [41,42].…”
Section: Jhep03(2016)065supporting
confidence: 73%
See 1 more Smart Citation
“…(2.5), (2.6) reproduce the known results for heavy quark-antiquark (squark-antisquark) pair-production soft anomalous dimension [32,33,[38][39][40] in the limit p B → 0. Also, our result for Γ qq→klB agrees with the result obtained in the SCET framework in [41,42].…”
Section: Jhep03(2016)065supporting
confidence: 73%
“…The evolution of the colour exchange at NLL is governed by the one-loop soft anomalous dimension [28,[32][33][34][35][36]. Starting from four coloured partons in the process, the soft anomalous dimension is a matrix and is known for heavyquark [32,33,37], dijet [34][35][36] and supersymmetric particle production [38][39][40]43], as well as for the general case of 2 → n QCD processes [28][29][30]. Here we adopt the calculations of the soft anomalous dimension for the case of 2 → 3 processes with two coloured massive particles in the final state.…”
Section: Jhep03(2016)065mentioning
confidence: 99%
“…Only the first two generations of squarks are considered, and they are assumed to be degenerate in mass. Signal cross sections are calculated to next-to-leading order in the strong coupling constant including the resummation of soft gluon emission at nextto-leading-logarithm accuracy when available [46][47][48][49][50]. The nominal cross section and its uncertainty are taken from an envelope of cross-section predictions using different PDF sets and factorization and renormalization scales, as described in Ref.…”
Section: Monte Carlo Simulation Samplesmentioning
confidence: 99%
“…The inclusion of the resummation of soft gluon emission at next-to-leading-logarithmic (NLL) accuracy (NLO þ NLL) [49][50][51][52][53] is performed in the case of strong sparticle pair production. For neutralino, chargino, slepton and sneutrino production, the NLO cross sections used are in agreement with the NLO þ NLL calculation within ∼2% [54][55][56].…”
Section: Monte Carlo Simulationsmentioning
confidence: 99%