2006
DOI: 10.1103/physrevd.74.013008
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Single top-quark production in thet- channel at CERN LHC: A realistic test of electroweak models

Abstract: We compute the complete electroweak one-loop effect on the process of t-channel single top production at LHC in the Standard Model and in the MSSM within the mSUGRA symmetry breaking scheme. We find that the one-loop electroweak SM effect is large, and decreases the cross section of an amount that is of the same size as that of the NLO QCD one. The genuine SUSY effect in the mSUGRA scheme, for a general choice of benchmark points, is rather small.It might become large and visible in more general scenarios arou… Show more

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Cited by 23 publications
(11 citation statements)
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References 41 publications
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“…1(a)). This extends previous NLO (QCD or EW) results which are based on the 2 → 2 leading order process [19,20,21,22,23,24,25,26,27]. A comparison of the two calculations allows a first study of their consistency across a broad kinematic range.…”
Section: Introductionsupporting
confidence: 75%
“…1(a)). This extends previous NLO (QCD or EW) results which are based on the 2 → 2 leading order process [19,20,21,22,23,24,25,26,27]. A comparison of the two calculations allows a first study of their consistency across a broad kinematic range.…”
Section: Introductionsupporting
confidence: 75%
“…(6.22) includes both t-and s-channel mechanisms. Its NLO EW corrections have been computed before in the context of supersymmetric extensions of the SM [163][164][165] (a soft approximation has been employed in ref. [163] to deal with real-emission contributions).…”
Section: Associated Top-quark and Jet Productionmentioning
confidence: 99%
“…On the other hand, we will investigate how the description of the data is affected by the theoretical details that enter the computation of single top observables. Specifically, we will pay attention to the inclusion of higher-order quantum chromodynamics (QCD) corrections [18][19][20][21][22][23], recently computed up to next-to-next-to-leading order (NNLO) accuracy [24][25][26]; to the effect of next-to-leading order (NLO) electroweak (EW) corrections [27][28][29]; and to the choice of the heavy flavour scheme. In this last respect we will restrict our analysis to NLO QCD, and compare the four-flavour scheme (4FS) [30], in which the bottom quark is treated as a massive final state and does not contribute to the proton wave-function, with the five-flavour scheme (5FS) [18], in which the bottom quark is treated as a light quark, perturbatively generated within the proton above a certain matching scale (often taken to be of the order of the bottom-quark pole mass).…”
Section: Introductionmentioning
confidence: 99%