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Single-top $t$-channel production with off-shell and non-resonant effects
High Energy Physics - Phenomenology · Submitted 30 May 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Results are presented for the LHC and compared to those of the narrow-width approximation and effective theory approaches.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
This letter details and discusses the next-to-leading order QCD corrections to $t$-channel electro-weak $W^+ b j$ production, where finite top-width effects are consistently taken into account. The computation is done within the aMC@NLO framework and includes both resonant and non-resonant contributions as well as interferences between the two. Results are presented for the LHC and compared to those of the narrow-width approximation and effective theory approaches.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | This letter details and discusses the next-to-leading order QCD corrections to $t$-channel electro-weak $W^+ b j$ production, where finite top-width effects are consistently taken into account. | contribution 1.00 | 0.89 | 0.16 | asserted 0.98 |
| s1 | The computation is done within the aMC@NLO framework and includes both resonant and non-resonant contributions as well as interferences between the two. | method 0.99 | 0.93 | 0.08 | asserted 1.00 |
| s2 | Results are presented for the LHC and compared to those of the narrow-width approximation and effective theory approaches. | result 0.76 | 0.89 | 0.15 | asserted 0.98 |
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The paper
Original abstract
This letter details and discusses the next-to-leading order QCD corrections to $t$-channel electro-weak $W^+ b j$ production, where finite top-width effects are consistently taken into account. The computation is done within the aMC@NLO framework and includes both resonant and non-resonant contributions as well as interferences between the two. Results are presented for the LHC and compared to those of the narrow-width approximation and effective theory approaches.
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References
How the literature uses it
14 arXiv papers cite this in 29 sentences
Papers citing it · 13 sentences without a confident label
Uses its method or tool 1 paper
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The first gauge invariant calculation valid also in the far off-shell region was performed [ref] in the complex mass scheme [ref] , and this is the approach we follow.
Off-shell single-top-quark production in the Standard Model Effective Field Theory · Introduction · 0.90
Compares with it 2 papers
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In order to directly compare our present results to previous work at fNLO [ref] , and to ensure that the conclusions presented below at the hadron level are in as close analogy as possible with those of ref.
Off-shell single-top production at NLO matched to parton showers · Single-top hadroproduction: process definition and approximations · 1.00
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[ref] with an on-shell $W$-boson seems to obtain a smooth $m_t$ distribution with 1 bins without applying any smearing procedures.
Off-shell single-top-quark production in the Standard Model Effective Field Theory · Off-shell and $W$-reconstruction effects in the Standard Model. · 0.80
Cites it as support 1 paper
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NLO corrections to the decay become important near the peak of the distribution, whilst at the peak and above it becomes crucial to treat the top quark as off-shell [ref] .
Off-shell single-top production at NLO matched to parton showers · Relative transverse momentum of primary $b$-jet, $p_T,rel(J_b)$ · 0.97
Cites it as background 5 papers
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Full NLO corrections including top-quark leptonic decay are studied within the on-shell top-quark approximation [ref] and beyond [ref] .
Top-quark mass determination from t-channel single top production at the LHC · Introduction · 0.92
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Significant efforts have been made in this direction at next-to-leading order (NLO), both treating the top-quark propagator in the narrow-width approximation (NWA) [ref] as well as keeping the top quarks off their mass-shell [ref] .
Top-quark pair-production and decay at high precision · Introduction · 0.92
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Off-shell top-quark effects have also been considered at NLO, both at fixed order [ref] and further in the context of NLO parton shower matched simulations [ref] .
MINLO t-channel single-top plus jet · Introduction · 0.95
What it cites · 44 sentences without a confident label
Uses the method or tool of 5 papers
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The NLO corrections have thus been obtained in an automated fashion, with the one-loop and real contributions computed using MadLoop [ref] and MadFKS [ref] respectively.
Automation of next-to-leading order computations in QCD: the FKS subtraction · Unstable single-top production · 1.00
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The NLO corrections have thus been obtained in an automated fashion, with the one-loop and real contributions computed using MadLoop [ref] and MadFKS [ref] respectively.
Automation of one-loop QCD corrections · Unstable single-top production · 1.00
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We thank the authors of [ref] for providing us with their code for the ET results.
Production-decay interferences at NLO in QCD for t-channel single-top production · Acknowledgements · 0.98
Cites as background 16 papers
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Going beyond the NWA, a study of off-shell and non-resonant effects at LO was performed in [ref] and final-state non-factorizable corrections in the $s$-channel were examined in [ref] .
Final state QCD corrections to off-shell single top production in hadron collisions · Introduction · 0.86
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Going beyond the NWA, a study of off-shell and non-resonant effects at LO was performed in [ref] and final-state non-factorizable corrections in the $s$-channel were examined in [ref] .
Helicity Amplitudes for Single-Top Production · Introduction · 0.86
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Next-to-leading order (NLO) QCD corrections in the five-flavour (5F) scheme were first computed in [ref] and in the four-flavour (4F) scheme in [ref] , whilst electro-weak (EW) corrections were investigated in [ref] .
The fully differential single-top-quark cross section in next-to-leading order QCD · Introduction · 0.98
Discussion
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