pith. sign in

arxiv: 2606.19999 · v1 · pith:47SHUFGGnew · submitted 2026-06-18 · ✦ hep-ph · hep-ex

NLO QCD and EW corrections to semileptonic vector-boson scattering at the LHC

Pith reviewed 2026-06-26 17:09 UTC · model grok-4.3

classification ✦ hep-ph hep-ex
keywords vector-boson scatteringNLO correctionselectroweakQCDsemileptonicLHCfiducial cross sectionsdifferential distributions
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0 comments X

The pith

Fully off-shell NLO QCD and EW corrections are computed for semileptonic vector-boson scattering at the LHC.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper computes the next-to-leading order corrections in QCD and the electroweak sector for the semileptonic vector-boson scattering process at the LHC. The calculation is performed in a fully off-shell manner for the process producing a lepton, neutrino and four jets. It focuses on the leading electroweak contribution at order alpha to the sixth power along with its corrections at order alpha to the seventh and the mixed alpha_s alpha to the sixth. Results are presented for cross sections and distributions in two fiducial regions selected for their relevance to vector-boson scattering. Such predictions are essential as experimental measurements of this process become more precise.

Core claim

In a fully off-shell calculation, we provide results for the leading electroweak contribution of O(α^6) and the corresponding corrections of O(α^7) and O(α_s α^6) for fiducial cross sections and a selection of differential distributions in the process pp → ℓ⁺ ν_ℓ + 4j in two different fiducial regions relevant for vector-boson scattering.

What carries the argument

Fully off-shell NLO calculation of electroweak and QCD corrections to the semileptonic vector-boson scattering process pp → ℓ⁺ ν_ℓ + 4j

If this is right

  • The provided NLO results enable more precise comparisons with LHC data on vector-boson scattering.
  • Corrections of O(α^7) and O(α_s α^6) modify the leading O(α^6) predictions for cross sections.
  • Differential distributions in the fiducial regions can be directly compared to experimental measurements.
  • The calculation covers both QCD and electroweak corrections for improved accuracy.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The method could be applied to fully leptonic or other decay channels of vector-boson scattering.
  • Including these corrections may reduce theoretical uncertainties in VBS analyses at the LHC.
  • The fiducial region definitions could be optimized based on these theoretical results.

Load-bearing premise

The two chosen fiducial regions sufficiently isolate the vector-boson scattering signal and that the perturbative series truncated at NLO remains a reliable approximation inside those regions.

What would settle it

Experimental measurement of the fiducial cross section or distributions in the two regions that significantly deviates from the NLO theoretical prediction after accounting for these corrections.

read the original abstract

Vector-boson scattering with semileptonic final states has recently been measured at the LHC, and future experiments are expected to further increase the precision of its measurement, calling for adequate theoretical predictions. In this work, we present a calculation of the NLO QCD and electroweak corrections to the process $\text{p}\text{p} \to \ell^+ \nu_\ell + 4\text{j}$ in two different fiducial regions relevant for vector-boson scattering. In a fully off-shell calculation, we provide results for the leading electroweak contribution of $\mathcal{O}\left(\alpha^6\right)$ and the corresponding corrections of $\mathcal{O}\left(\alpha^7\right)$ and $\mathcal{O}\left(\alpha_\text{s} \alpha^6\right)$ for fiducial cross sections and a selection of differential distributions.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The paper presents a fully off-shell calculation of NLO QCD and electroweak corrections to the semileptonic vector-boson scattering process pp → ℓ⁺ν_ℓ + 4j at the LHC. It computes the leading electroweak contribution at O(α⁶) together with the NLO corrections at O(α⁷) and O(α_s α⁶) for fiducial cross sections and selected differential distributions in two fiducial regions chosen to isolate the VBS signal.

Significance. If the results hold, the work supplies important higher-order predictions for a process that has been measured at the LHC and will be measured with greater precision. The explicit Feynman-diagram evaluation in the Standard Model and the fully off-shell treatment constitute a clear computational strength for this class of calculations.

major comments (1)
  1. [Numerical results section] Numerical results section: the manuscript supplies no explicit check—such as the relative size of the NLO corrections versus LO across the reported distributions or an estimate of missing NNLO pieces—to confirm that the perturbative series truncated at NLO remains reliable inside the chosen fiducial regions. This assumption is load-bearing for the applicability of the central claim.

Simulated Author's Rebuttal

1 responses · 1 unresolved

We thank the referee for the positive evaluation of the computational approach and for highlighting the need for explicit checks on perturbative reliability. We address the major comment below.

read point-by-point responses
  1. Referee: [Numerical results section] Numerical results section: the manuscript supplies no explicit check—such as the relative size of the NLO corrections versus LO across the reported distributions or an estimate of missing NNLO pieces—to confirm that the perturbative series truncated at NLO remains reliable inside the chosen fiducial regions. This assumption is load-bearing for the applicability of the central claim.

    Authors: We agree that explicit verification of the size of the NLO corrections is necessary to support the applicability of the results. In the revised manuscript we will add tables and/or figures displaying the relative NLO QCD and EW corrections (K-factors) with respect to the LO predictions for the fiducial cross sections and for all reported differential distributions in both fiducial regions. This will directly quantify the corrections inside the selected phase-space regions. For an estimate of missing NNLO pieces we will include a discussion based on the observed NLO scale uncertainties and on comparisons with existing higher-order studies of related VBS processes; a dedicated NNLO calculation lies outside the scope of the present work. revision: yes

standing simulated objections not resolved
  • A precise quantitative estimate of missing NNLO contributions without performing a full NNLO calculation

Circularity Check

0 steps flagged

No significant circularity; explicit Feynman-diagram computation in SM

full rationale

The paper computes LO O(α^6) and NLO O(α^7), O(α_s α^6) corrections to pp → ℓ⁺ν_ℓ + 4j via direct evaluation of Feynman diagrams in the Standard Model for two fiducial regions. No load-bearing step reduces to a fitted parameter, self-definition, or self-citation chain; the central results are obtained from explicit diagrammatic evaluation rather than by construction from inputs. The assumption that NLO truncation is reliable inside the regions is an external validity claim, not a circular reduction of the reported numbers. This is the normal case of a self-contained perturbative calculation.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The work rests on the Standard Model perturbative expansion and standard choices for scales and parton distributions; no new entities or ad-hoc assumptions beyond those common to NLO phenomenology are introduced.

free parameters (1)
  • renormalization and factorization scales
    Standard choice in NLO calculations to estimate missing higher orders; values not specified in abstract.
axioms (1)
  • standard math Standard Model Feynman rules and perturbative expansion
    The calculation is performed within the SM at fixed orders in α and α_s.

pith-pipeline@v0.9.1-grok · 5688 in / 965 out tokens · 33464 ms · 2026-06-26T17:09:08.224338+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

76 extracted references · 1 canonical work pages

  1. [1]

    [3]CMScollaboration,First measurements of vector boson scattering inW ±W ± and WZ production in all-leptonic final states at√s= 13.6 TeV,2605.15396

    ATLAScollaboration,Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at√s=13TeV with the ATLAS detector,JHEP04 (2024) 026 [2312.00420]. [3]CMScollaboration,First measurements of vector boson scattering inW ±W ± and WZ production in all-leptonic final states at√s= 13.6 TeV,2605.15396

  2. [2]

    CMScollaboration,Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets in proton-proton collisions at√s=13TeV,Phys. Lett. B809 (2020) 135710 [2005.01173]. [5]ATLAScollaboration,Measurements of electroweakW ±Zboson pair production in association with two jets inppcollisions at√s=13TeV with the ATLAS detec...

  3. [3]

    – 23 – [8]CMScollaboration,Measurement of the electroweak production of Wγin association with two jets in proton-proton collisions at√s=13TeV,Phys

    ATLAScollaboration,Differential cross-section measurements of the production of four charged leptons in association with two jets using the ATLAS detector,JHEP01(2024) 004 [2308.12324]. – 23 – [8]CMScollaboration,Measurement of the electroweak production of Wγin association with two jets in proton-proton collisions at√s=13TeV,Phys. Rev. D108(2023) 032017 ...

  4. [4]

    ATLAScollaboration,Fiducial and differential cross-section measurements of electroweakWγjj production inpp collisions at√s =13TeV with the ATLAS detector,Eur. Phys. J. C84(2024) 1064 [2403.02809]. [10]CMScollaboration,Measurement of the electroweak production of Zγand two jets in proton-proton collisions at√s=13TeV and constraints on anomalous quartic gau...

  5. [5]

    ATLAScollaboration,Measurement of the cross-sections of the electroweak and total production of aZγpair in association with two jets inppcollisions at√s= 13 TeV with the ATLAS detector,Phys. Lett. B846(2023) 138222 [2305.19142]. [12]CMScollaboration,Observation of electroweakW +W − pair production in association with two jets in proton-proton collisions a...

  6. [6]

    [14]CMScollaboration,Measurements of production cross sections of polarized same-sign W boson pairs in association with two jets in proton-proton collisions at√s=13TeV,Phys

    ATLAScollaboration,Observation of electroweak production ofW +W − in association with jets in proton-proton collisions at√s=13TeV with the ATLAS Detector,JHEP07(2024) 254 [2403.04869]. [14]CMScollaboration,Measurements of production cross sections of polarized same-sign W boson pairs in association with two jets in proton-proton collisions at√s=13TeV,Phys...

  7. [7]

    [18]ATLAScollaboration,Observation of gauge boson joint-polarisation states inW ±Zproduction fromppcollisions at √s= 13TeV with the ATLAS detector,Phys

    CMScollaboration,Measurement of the inclusive and differential WZ production cross sections, polarization angles, and triple gauge couplings in pp collisions at√s=13TeV,JHEP07(2022) 032 [2110.11231]. [18]ATLAScollaboration,Observation of gauge boson joint-polarisation states inW ±Zproduction fromppcollisions at √s= 13TeV with the ATLAS detector,Phys. Lett...

  8. [8]

    ATLAScollaboration,Studies of the Energy Dependence of Diboson Polarization Fractions and the Radiation-Amplitude-Zero Effect in WZ Production with the ATLAS Detector,Phys. Rev. Lett.133(2024) 101802 [2402.16365]. [20]ATLAScollaboration,Evidence of pair production of longitudinally polarised vector bosons and study of CP properties in ZZ→4ℓevents with the...

  9. [9]

    Jäger, C

    B. Jäger, C. Oleari and D. Zeppenfeld,Next-to-leading order QCD corrections toW+W − production via vector-boson fusion,JHEP07(2006) 015 [hep-ph/0603177]

  10. [10]

    Jäger, C

    B. Jäger, C. Oleari and D. Zeppenfeld,Next-to-leading order QCD corrections to Z boson pair production via vector-boson fusion,Phys. Rev. D73(2006) 113006 [hep-ph/0604200]

  11. [11]

    Bozzi, B

    G. Bozzi, B. Jäger, C. Oleari and D. Zeppenfeld,Next-to-leading order QCD corrections toW +Z and W −Z production via vector-boson fusion,Phys. Rev. D75(2007) 073004 [hep-ph/0701105]

  12. [12]

    Jäger, C

    B. Jäger, C. Oleari and D. Zeppenfeld,Next-to-leading order QCD corrections toW +W +jj and W −W −jjproduction via weak-boson fusion,Phys. Rev. D80(2009) 034022 [0907.0580]

  13. [13]

    Denner, L

    A. Denner, L. Hošeková and S. Kallweit,NLO QCD corrections toW+W +jj production in vector-boson fusion at the LHC,Phys. Rev. D86(2012) 114014 [1209.2389]

  14. [14]

    Rauch,Vector-Boson Fusion and Vector-Boson Scattering,1610.08420

    M. Rauch,Vector-Boson Fusion and Vector-Boson Scattering,1610.08420

  15. [15]

    Melia, K

    T. Melia, K. Melnikov, R. Röntsch and G. Zanderighi,Next-to-leading order QCD predictions for W +W +jjproduction at the LHC,JHEP12(2010) 053 [1007.5313]

  16. [16]

    Melia, K

    T. Melia, K. Melnikov, R. Röntsch and G. Zanderighi,NLO QCD corrections forW+W − pair production in association with two jets at hadron colliders,Phys. Rev. D83(2011) 114043 [1104.2327]

  17. [17]

    Greiner, G

    N. Greiner, G. Heinrich, P. Mastrolia, G. Ossola, T. Reiter and F. Tramontano,NLO QCD corrections to the production ofW+W − plus two jets at the LHC,Phys. Lett. B713(2012) 277 [1202.6004]

  18. [18]

    Campanario, M

    F. Campanario, M. Kerner, L.D. Ninh and D. Zeppenfeld,WZ Production in Association with Two Jets at Next-to-Leading Order in QCD,Phys. Rev. Lett.111(2013) 052003 [1305.1623]

  19. [19]

    Campanario, M

    F. Campanario, M. Kerner, L.D. Ninh and D. Zeppenfeld,Next-to-leading order QCD corrections to ZZ production in association with two jets,JHEP07(2014) 148 [1405.3972]

  20. [20]

    Campanario, M

    F. Campanario, M. Kerner, L.D. Ninh and D. Zeppenfeld,Next-to-leading order QCD corrections toWγproduction in association with two jets,Eur. Phys. J. C74(2014) 2882 [1402.0505]

  21. [21]

    Ballestrero et al.,Precise predictions for same-sign W-boson scattering at the LHC,Eur

    A. Ballestrero et al.,Precise predictions for same-sign W-boson scattering at the LHC,Eur. Phys. J. C78(2018) 671 [1803.07943]

  22. [22]

    Jäger and G

    B. Jäger and G. Zanderighi,NLO corrections to electroweak and QCD production ofW +W + plus two jets in the POWHEGBOX,JHEP11(2011) 055 [1108.0864]

  23. [23]

    Jäger and G

    B. Jäger and G. Zanderighi,ElectroweakW+W −jjprodution at NLO in QCD matched with parton shower in the POWHEG-BOX,JHEP04(2013) 024 [1301.1695]. – 25 –

  24. [24]

    Jäger, A

    B. Jäger, A. Karlberg and G. Zanderighi,ElectroweakZZjjproduction in the Standard Model and beyond in the POWHEG-BOX V2,JHEP03(2014) 141 [1312.3252]

  25. [25]

    Rauch and S

    M. Rauch and S. Plätzer,Parton Shower Matching Systematics in Vector-Boson-Fusion WW Production,Eur. Phys. J. C77(2017) 293 [1605.07851]

  26. [26]

    Rauch and S

    M. Rauch and S. Plätzer,Parton-shower Effects in Vector-Boson-Fusion Processes,PoS DIS2016(2016) 076 [1607.00159]

  27. [27]

    Jäger, A

    B. Jäger, A. Karlberg and J. Scheller,Parton-shower effects in electroweakWZjjproduction at the next-to-leading order of QCD,Eur. Phys. J. C79(2019) 226 [1812.05118]

  28. [28]

    Jäger, A

    B. Jäger, A. Karlberg and S. Reinhardt,QCD effects in electroweakWZjj production at current and future hadron colliders,Eur. Phys. J. C84(2024) 587 [2403.12192]

  29. [29]

    Melia, P

    T. Melia, P. Nason, R. Röntsch and G. Zanderighi,W+W −, WZ and ZZ production in the POWHEG BOX,JHEP11(2011) 078 [1107.5051]

  30. [30]

    Baglio et al.,Release Note - VBFNLO 2.7.0,1404.3940

    J. Baglio et al.,Release Note - VBFNLO 2.7.0,1404.3940

  31. [31]

    Stelzer and W.F

    T. Stelzer and W.F. Long,Automatic generation of tree level helicity amplitudes,Comput. Phys. Commun.81(1994) 357 [hep-ph/9401258]

  32. [32]

    Alwall, R

    J. Alwall, R. Frederix, S. Frixione, V. Hirschi, F. Maltoni, O. Mattelaer et al.,The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations,JHEP07(2014) 079 [1405.0301]. [49]Sherpacollaboration,Event Generation with Sherpa 2.2,SciPost Phys.7(2019) 034 [1905.09127]

  33. [33]

    Nason,A new method for combining NLO QCD with shower Monte Carlo algorithms,JHEP 11(2004) 040 [hep-ph/0409146]

    P. Nason,A new method for combining NLO QCD with shower Monte Carlo algorithms,JHEP 11(2004) 040 [hep-ph/0409146]

  34. [34]

    Frixione, P

    S. Frixione, P. Nason and C. Oleari,Matching NLO QCD computations with Parton Shower simulations: the POWHEG method,JHEP11(2007) 070 [0709.2092]

  35. [35]

    Alioli, P

    S. Alioli, P. Nason, C. Oleari and E. Re,A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX,JHEP06(2010) 043 [1002.2581]

  36. [36]

    Biedermann, A

    B. Biedermann, A. Denner and M. Pellen,Large electroweak corrections to vector-boson scattering at the Large Hadron Collider,Phys. Rev. Lett.118(2017) 261801 [1611.02951]

  37. [37]

    Denner, S

    A. Denner, S. Dittmaier, P. Maierhöfer, M. Pellen and C. Schwan,QCD and electroweak corrections to WZ scattering at the LHC,JHEP06(2019) 067 [1904.00882]

  38. [38]

    Denner, R

    A. Denner, R. Franken, M. Pellen and T. Schmidt,NLO QCD and EW corrections to vector-boson scattering into ZZ at the LHC,JHEP11(2020) 110 [2009.00411]

  39. [39]

    Denner, R

    A. Denner, R. Franken, T. Schmidt and C. Schwan,NLO QCD and EW corrections to vector-boson scattering intoW+W − at the LHC,JHEP06(2022) 098 [2202.10844]

  40. [40]

    Biedermann, A

    B. Biedermann, A. Denner and M. Pellen,Complete NLO corrections toW+W + scattering and its irreducible background at the LHC,JHEP10(2017) 124 [1708.00268]

  41. [41]

    Denner, R

    A. Denner, R. Franken, M. Pellen and T. Schmidt,Full NLO predictions for vector-boson scattering into Z bosons and its irreducible background at the LHC,JHEP10(2021) 228 [2107.10688]. – 26 –

  42. [42]

    Denner, D

    A. Denner, D. Lombardi, S. Lopez Portillo Chavez, M. Pellen and G. Pelliccioli,MoCaNLO: a Monte Carlo integrator for NLO calculations,2602.19842

  43. [43]

    Denner, D

    A. Denner, D. Lombardi, S. Lopez Portillo Chavez, M. Pellen and G. Pelliccioli,Mocanlo, Feb.,

  44. [44]

    10.5281/zenodo.19829093

  45. [45]

    Chiesa, A

    M. Chiesa, A. Denner, J.-N. Lang and M. Pellen,An event generator for same-sign W-boson scattering at the LHC including electroweak corrections,Eur. Phys. J. C79(2019) 788 [1906.01863]

  46. [46]

    Ballestrero, E

    A. Ballestrero, E. Maina and G. Pelliccioli,Different polarization definitions in same-signWW scattering at the LHC,Phys. Lett. B811(2020) 135856 [2007.07133]

  47. [47]

    Ballestrero, E

    A. Ballestrero, E. Maina and G. Pelliccioli,W boson polarization in vector boson scattering at the LHC,JHEP03(2018) 170 [1710.09339]

  48. [48]

    Ballestrero, E

    A. Ballestrero, E. Maina and G. Pelliccioli,Polarized vector boson scattering in the fully leptonic WZ and ZZ channels at the LHC,JHEP09(2019) 087 [1907.04722]

  49. [49]

    Buarque Franzosi, O

    D. Buarque Franzosi, O. Mattelaer, R. Ruiz and S. Shil,Automated predictions from polarized matrix elements,JHEP04(2020) 082 [1912.01725]

  50. [50]

    Denner, C

    A. Denner, C. Haitz and G. Pelliccioli,NLO EW and QCD corrections to polarised same-sign WW scattering at the LHC,JHEP11(2024) 115 [2409.03620]

  51. [51]

    Denner, R

    A. Denner, R. Franken, C. Haitz, D. Lombardi and G. Pelliccioli,Electroweak corrections to doubly polarised WZ scattering at the LHC,JHEP02(2026) 120 [2510.26462]

  52. [52]

    Ballestrero, G

    A. Ballestrero, G. Bevilacqua and E. Maina,A Complete parton level analysis of boson-boson scattering and ElectroWeak Symmetry Breaking inℓν+ four jets production at the LHC,JHEP 05(2009) 015 [0812.5084]

  53. [53]

    Denner, D

    A. Denner, D. Lombardi and C. Schwan,Double-pole approximation for leading-order semi-leptonic vector-boson scattering at the LHC,JHEP08(2024) 146 [2406.12301]

  54. [54]

    Denner, S

    A. Denner, S. Dittmaier, M. Roth and L.H. Wieders,Electroweak corrections to charged-current e+e−→4 fermion processes: Technical details and further results,Nucl. Phys.B724(2005) 247 [hep-ph/0505042]

  55. [55]

    Denner, S

    A. Denner, S. Dittmaier, M. Roth and D. Wackeroth,Electroweak radiative corrections to e+e−→WW→4 fermions in double pole approximation: The RACOONWW approach,Nucl. Phys.B587(2000) 67 [hep-ph/0006307]

  56. [56]

    Catani and M.H

    S. Catani and M.H. Seymour,A general algorithm for calculating jet cross-sections in NLO QCD, Nucl. Phys.B485(1997) 291 [hep-ph/9605323]

  57. [57]

    Dittmaier,A general approach to photon radiation off fermions,Nucl

    S. Dittmaier,A general approach to photon radiation off fermions,Nucl. Phys.B565(2000) 69 [hep-ph/9904440]

  58. [58]

    Catani, S

    S. Catani, S. Dittmaier, M.H. Seymour and Z. Trócsányi,The dipole formalism for next-to-leading order QCD calculations with massive partons,Nucl. Phys.B627(2002) 189 [hep-ph/0201036]

  59. [59]

    Dittmaier, A

    S. Dittmaier, A. Kabelschacht and T. Kasprzik,Polarized QED splittings of massive fermions and dipole subtraction for non-collinear-safe observables,Nucl. Phys.B800(2008) 146 [0802.1405]

  60. [60]

    Actis, A

    S. Actis, A. Denner, L. Hofer, A. Scharf and S. Uccirati,Recursive generation of one-loop amplitudes in the Standard Model,JHEP04(2013) 037 [1211.6316]. – 27 –

  61. [61]

    Denner, S

    A. Denner, S. Dittmaier and L. Hofer,COLLIER: a fortran-based Complex One-Loop LIbrary in Extended Regularizations,Comput. Phys. Commun.212(2017) 220 [1604.06792]

  62. [62]

    Berends, R

    F.A. Berends, R. Pittau and R. Kleiss,All electroweak four fermion processes in electron-positron collisions,Nucl. Phys.B424(1994) 308 [hep-ph/9404313]

  63. [63]

    Denner, S

    A. Denner, S. Dittmaier, M. Roth and D. Wackeroth,Predictions for all processese+e−→4 fermions+γ,Nucl. Phys.B560(1999) 33 [hep-ph/9904472]

  64. [64]

    Dittmaier and M

    S. Dittmaier and M. Roth,LUSIFER: A LUcid approach to six FERmion production,Nucl. Phys. B642(2002) 307 [hep-ph/0206070]

  65. [65]

    Nagy,Next-to-leading order calculation of three jet observables in hadron hadron collision, Phys

    Z. Nagy,Next-to-leading order calculation of three jet observables in hadron hadron collision, Phys. Rev. D68(2003) 094002 [hep-ph/0307268]. [82]Particle Data Groupcollaboration,Review of particle physics,Phys. Rev. D110(2024) 030001. [83]LHC Higgs Cross Section Working Groupcollaboration,Handbook of LHC Higgs Cross Sections: 3. Higgs Properties, (Geneva)...

  66. [66]

    Andersen et al.,Les Houches 2013: Physics at TeV Colliders: Standard Model Working Group Report, 2014 [1405.1067]

    J.R. Andersen et al.,Les Houches 2013: Physics at TeV Colliders: Standard Model Working Group Report, 2014 [1405.1067]

  67. [67]

    Buckley, J

    A. Buckley, J. Ferrando, S. Lloyd, K. Nordström, B. Page, M. Rüfenacht et al.,LHAPDF6: parton density access in the LHC precision era,Eur. Phys. J.C75(2015) 132 [1412.7420]. [87]ATLAScollaboration,Prospective study of vector boson scattering in WZ fully leptonic final state at HL-LHC, ATL-PHYS-PUB-2018-023. [88]CMScollaboration,Evidence for WW/WZ vector b...

  68. [68]

    Dokshitzer, G.D

    Y.L. Dokshitzer, G.D. Leder, S. Moretti and B.R. Webber,Better jet clustering algorithms, JHEP08(1997) 001 [hep-ph/9707323]

  69. [69]

    Wobisch and T

    M. Wobisch and T. Wengler,Hadronization corrections to jet cross-sections in deep inelastic scattering, inWorkshop on Monte Carlo Generators for HERA Physics (Plenary Starting Meeting), pp. 270–279, 4, 1998 [hep-ph/9907280]

  70. [70]

    Cacciari, G.P

    M. Cacciari, G.P. Salam and G. Soyez,The anti-kt jet clustering algorithm,JHEP04(2008) 063 [0802.1189]

  71. [71]

    Denner and S

    A. Denner and S. Pozzorini,One loop leading logarithms in electroweak radiative corrections

  72. [72]

    Results,Eur. Phys. J.C18(2001) 461 [hep-ph/0010201]

  73. [73]

    Accomando, A

    E. Accomando, A. Denner and S. Pozzorini,Logarithmic electroweak corrections to e+e−→νe¯νeW +W −,JHEP03(2007) 078 [hep-ph/0611289]

  74. [74]

    Pagani and M

    D. Pagani and M. Zaro,One-loop electroweak Sudakov logarithms: a revisitation and automation, JHEP02(2022) 161 [2110.03714]

  75. [75]

    Lindert and L

    J.M. Lindert and L. Mai,Logarithmic EW corrections at one-loop,Eur. Phys. J. C84(2024) 1084 [2312.07927]. – 28 –

  76. [76]

    Denner and S

    A. Denner and S. Rode,Automated resummation of electroweak Sudakov logarithms in diboson production at future colliders,Eur. Phys. J. C84(2024) 542 [2402.10503]. – 29 –