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Next-to-leading order corrections to Wt production and decay
High Energy Physics - Phenomenology · Submitted 28 Jun 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that, for a choice of scale which is suitable for this approach, the QCD corrections are very mild and only change the cross section by up to 10% at the LHC, depending on the severity of the b-jet veto.
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The abstract, sentence by sentence
We present the results of a next-to-leading order calculation of Wt production, including the decays of both the top quark and the W boson. The effects of radiation in the decay of the top quark are also included. The separation of diagrams which appear in the real corrections, into singly- and doubly-resonant contributions, is performed using a b-jet veto which is motivated by the use of the bottom quark distribution function. We find that, for a choice of scale which is suitable for this approach, the QCD corrections are very mild and only change the cross section by up to 10% at the LHC, depending on the severity of the b-jet veto. When further cuts are applied, applicable for a Higgs boson search in the H->WW channel, we find that the radiative effects greatly decrease the number of background events expected from this process. In addition, the shapes of relevant distributions can be significantly changed at next-to-leading order.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present the results of a next-to-leading order calculation of Wt production, including the decays of both the top quark and the W boson. | contribution 1.00 | 0.96 | 0.11 | asserted 0.99 |
| s1 | The effects of radiation in the decay of the top quark are also included. | contribution 0.72 | 0.84 | 0.03 | asserted 1.00 |
| s2 | The separation of diagrams which appear in the real corrections, into singly- and doubly-resonant contributions, is performed using a b-jet veto which is motivated by the use of the bottom quark distribution function. | method 1.00 | 0.90 | 0.04 | asserted 1.00 |
| s3 | We find that, for a choice of scale which is suitable for this approach, the QCD corrections are very mild and only change the cross section by up to 10% at the LHC, depending on the severity of the b-jet veto. | result 1.00 | 0.97 | 0.49 | asserted 1.00 |
| s4 | When further cuts are applied, applicable for a Higgs boson search in the H->WW channel, we find that the radiative effects greatly decrease the number of background events expected from this process. | result 0.97 | 0.96 | 0.15 | asserted 1.00 |
| s5 | In addition, the shapes of relevant distributions can be significantly changed at next-to-leading order. | result 1.00 | 0.89 | 0.12 | asserted 0.90 |
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The paper
Original abstract
We present the results of a next-to-leading order calculation of Wt production, including the decays of both the top quark and the W boson. The effects of radiation in the decay of the top quark are also included. The separation of diagrams which appear in the real corrections, into singly- and doubly-resonant contributions, is performed using a b-jet veto which is motivated by the use of the bottom quark distribution function. We find that, for a choice of scale which is suitable for this approach, the QCD corrections are very mild and only change the cross section by up to 10% at the LHC, depending on the severity of the b-jet veto. When further cuts are applied, applicable for a Higgs boson search in the H->WW channel, we find that the radiative effects greatly decrease the number of background events expected from this process. In addition, the shapes of relevant distributions can be significantly changed at next-to-leading order.
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References
How later papers used it
63 later papers cite it
2 later papers by other authors are listed below: 2 used its data or values.
Uses its data or values 2 of 6 papers with this label
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Used the inclusive single-top-quark associated production (tW) NLO cross section of 10.6±0.8 pb.
Measurement of the Top-antitop Production Cross Section in pp Collisions at sqrt(s)=7 TeV using the Kinematic Properties of Events with Leptons and Jets (2011) · 1.00 · paraphrased: the licence does not allow quoting
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Modeled electroweak single-top production in the tW channel using its 10.6 pb cross section.
First Measurement of the Cross Section for Top-Quark Pair Production in Proton-Proton Collisions at sqrt(s)=7 TeV (2010) · 0.80 · paraphrased: the licence does not allow quoting
How the literature uses it
60 arXiv papers cite this in 94 sentences
Papers citing it · 54 sentences without a confident label
Builds on it 1 paper
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In Refs. [ref] , the analysis has been extended by including the semileptonic decay of the top quark in the narrow-width approximation.
Top-Quark Physics at the LHC · Single Top-Quark Production · 0.95
Uses its method or tool 8 papers
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The cross section of the top production processes are calculated at NLO using MCFM 6.1 [ref] , while PYTHIA 8.1.53 [ref] is used for W+jets cross section.
Observability of s-channel Heavy Charged Higgs at LHC Using Top Tagging Technique · Signal and Background Events and their Cross Sections · 0.99
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[ref] , and discussed here in sect.
Single-top hadroproduction in association with a W boson · Transverse momentum veto · 0.86
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The NLO cross sections in the b-jet veto scheme are evaluated using MCFM [ref] with $p_T^b-jet<50$ GeV.
Momentum-space threshold resummation in $tW$ production at the LHC · Numerical results · 0.84
Uses its data or values 5 papers
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The t-channel single-top-quark NLO cross section (multiplied by the leptonic branching fraction of the W boson) has been determined as $σ_t = 21.0^+1.1_-1.0 pb$ using MCFM [ref] , where the uncertainty is defined similarly as for $tt̅$ production.
Measurement of the Top-antitop Production Cross Section in pp Collisions at sqrt(s)=7 TeV using the Kinematic Properties of Events with Leptons and Jets · Simulation of Signal and Background Events · 0.80
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Single top-quark and $VV$ samples are normalised to NLO inclusive cross sections calculated with [ref] .
Differential cross section measurements for the production of a W boson in association with jets in proton-proton collisions at sqrt(s) = 7 TeV · Data and simulation samples · 0.91
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The $t$-channel single top quark NLO cross section is $σ_t-ch. = 64.6^+3.4_-3.2$pb from mcfm [ref] .
Measurement of the top quark pair production cross section in pp collisions at sqrt(s) = 7 TeV in dilepton final states containing a tau · Event simulation · 0.96
Compares with it 1 paper
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The inclusive NLO cross section varies from 36.07(1) pb for $μ= 25$ GeV to 34.84(1) pb for $μ= 50$ GeV, 35.09(1) pb for $μ= 100$ GeV and 35.86(1) pb for $μ= 255$ GeV, thus showing a stability at the level of few per cent, in agreement with Figure 7 of Ref. [ref] .
A complete one-loop description of associated tW production at LHC and an estimate of possible genuine supersymmetric effects · NLO SM corrections · 0.96
Cites it as background 18 papers
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To date, the most precise full fixed-order prediction for $tW$ production is at next-to-leading order (NLO) in QCD [ref] .
Approximate N$^2$LO and N$^3$LO QCD Predictions for $tW$ Production · Introduction · 0.85
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Extensive studies of single top production at hadron colliders including radiative corrections have been performed at NLO [ref] and NNLO [ref] in the strong coupling.
Probing anomalous $Wtb$ couplings at the LHC in single top quark production through $t$-channel · Introduction · 0.92
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There, the suggestion was made to place a cut on the transverse momentum $^b$ of the “additional $b$ quark that appears at the next-to-leading order” [ref] , namely the $b$ quark that appears in the diagrams of fig.
Single-top hadroproduction in association with a W boson · Previous approaches · 0.80
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