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One-loop corrections to the Drell-Yan process in SANC (I). The charged current case
High Energy Physics - Phenomenology · Submitted 11 Jun 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Complete one-loop electroweak corrections are calculated within the automatic SANC system.
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The abstract, sentence by sentence
Radiative corrections to the charged current Drell-Yan processes are revisited. Complete one-loop electroweak corrections are calculated within the automatic SANC system. Electroweak scheme dependence and the choice of the factorization scale are discussed. Comparisons with earlier calculations are presented.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Radiative corrections to the charged current Drell-Yan processes are revisited. | background 0.53 | 0.68 | 0.06 | asserted 0.90 |
| s1 | Complete one-loop electroweak corrections are calculated within the automatic SANC system. | contribution 0.57 | 0.95 | 0.20 | asserted 1.00 |
| s2 | Electroweak scheme dependence and the choice of the factorization scale are discussed. | contribution 0.81 | 0.68 | 0.07 | asserted 0.77 |
| s3 | Comparisons with earlier calculations are presented. | contribution 0.78 | 0.76 | 0.07 | asserted 0.95 |
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The paper
Original abstract
Radiative corrections to the charged current Drell-Yan processes are revisited. Complete one-loop electroweak corrections are calculated within the automatic SANC system. Electroweak scheme dependence and the choice of the factorization scale are discussed. Comparisons with earlier calculations are presented.
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References
How the literature uses it
39 arXiv papers cite this in 52 sentences
Papers citing it · 25 sentences without a confident label
Builds on it 1 paper
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First, we presented in Ref. [ref] the CC case.
One-loop corrections to the Drell--Yan process in SANC (II). The neutral current case · Introduction · 0.93
Uses its method or tool 1 paper
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* step brdq, i.e. $(Δσ̂)^$, via call ProcessBrdq_(EW,QCD) (...,brdq,...) a) first part, i.e. $(Δσ̂^Virt+Soft)^$, * is computed by SSFM call cc$_$bo$_$xy$_$zv(...,born), multiplied by $(δ^SV)^$ — a CC analog of Eq.(19) of [ref] b) second part, i.e. $(dσ̂^Hard)^$ is computed by integration over $ξ$ of the function_(ew,qcd)_1s * and by SSFM call cc$_$bo$_$xy$_$zv(...,bornk), using Eq.(12) of [ref]
Standard SANC Modules · Overview of the packages · 0.91
Cites it as background 24 papers
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The complete $O(α)$ EW radiative corrections to $p p-7pt$^^(-)$ →W^± →ℓ^± ν$ ($ℓ=e, μ$) were calculated by several groups [ref] and found to agree [ref] .
Combining NLO QCD and Electroweak Radiative Corrections to W boson Production at Hadron Colliders in the POWHEG Framework · Introduction · 0.86
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The corrections up to $O(α)$ [ref] in the EW coupling are also available and are implemented in different public codes like [ref] , [ref] , [ref] , [ref] .
Precision Measurement of the W-Boson Mass: Theoretical Contributions and Uncertainties · Existing calculations and simulation codes · 0.80
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Concerning EW effects, the NLO corrections [ref] as well as leading higher-order effects from multiple photon emission and universal weak effects [ref] are known.
Dominant mixed QCD-electroweak $\mathcal{O}(\alpha_s\alpha)$ corrections to Drell-Yan processes in the resonance region · Introduction · 0.98
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