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Combining ATLAS vector-boson scattering and triboson data tightens limits on anomalous quartic gauge couplings from dimension-8 operators.

Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →

T0 review · grok-4.5

2026-07-15 11:53 UTC pith:77HC7ELO

load-bearing objection Solid ATLAS combination that delivers the first uniform 17-operator aQGC limits (unitarized and profiled) from seven VBS + one triboson channel; improvements of 17–96 % are real and usable.

arxiv 2603.18630 v2 pith:77HC7ELO submitted 2026-03-19 hep-ex

Combined effective field theory interpretation of measurements sensitive to quartic gauge boson couplings in pp collisions at sqrt{s}=13 TeV with the ATLAS detector

classification hep-ex
keywords anomalous quartic gauge couplingsdimension-8 EFTÉboli operatorsvector-boson scatteringtriboson productionATLASWilson coefficientsunitarity bounds
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved

The pith

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

This paper combines seven vector-boson scattering measurements and one triboson measurement, all using the full ATLAS Run-2 data set, into a single likelihood that constrains anomalous quartic electroweak gauge-boson couplings. Those couplings are parameterised by seventeen independent Wilson coefficients of dimension-8 operators in the Éboli effective-field-theory model. The combination produces 68 % and 95 % confidence intervals for each coefficient (and for selected pairs) both without and with unitarity constraints imposed by an energy-clipping procedure. The resulting unitarised intervals improve upon previously published ATLAS results by 17–96 % depending on the operator, and they remain competitive with analogous CMS limits. Simultaneous profiled fits that float all coefficients at once are also provided so that phenomenological models predicting correlated shifts can be tested directly.

Core claim

A joint likelihood built from seven VBS final states and one Wγγ triboson measurement yields the most comprehensive set of ATLAS constraints to date on the seventeen independent Éboli dimension-8 Wilson coefficients, with unitarised 95 % CL intervals that improve earlier ATLAS publications by up to 96 %.

What carries the argument

The combined profile-likelihood constructed from the individual analysis likelihoods, with nuisance parameters correlated where they share a common experimental origin and with EFT signal templates (linear, quadratic and cross terms) added to the SM prediction; unitarity is enforced by clipping the high-energy EFT contribution above a variable energy threshold and taking the intersection with theoretical unitarity bounds.

Load-bearing premise

Dimension-6 operators that can feed into the same final states through triple-gauge vertices are assumed already so tightly constrained that their residual effects can be set to zero.

What would settle it

A future global electroweak fit that finds a non-zero dimension-6 coefficient large enough to produce a measurable shift in any of the high-energy VBS or triboson distributions used here would bias or invalidate the reported dimension-8 intervals.

Watch this falsifier — get emailed when new claim-graph text bears on it.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

0 major / 5 minor

Summary. The ATLAS Collaboration combines seven vector-boson-scattering analyses and one tri-boson analysis (all based on 140 fb^{-1} of 13 TeV pp data) into a joint likelihood that constrains the 17 independent Wilson coefficients of the C-even, P-even dimension-8 operators of the Éboli basis that generate anomalous quartic gauge couplings. One- and two-dimensional 68 % and 95 % CL intervals are extracted both without unitarization and after energy-scale clipping that enforces partial-wave unitarity; positivity bounds are overlaid where available, and fully profiled simultaneous fits to all coefficients are also reported. The unitarized intervals improve the previously published ATLAS single-channel results by 17–96 % depending on the coefficient (Table 2).

Significance. If the reported intervals hold, the work supplies the most comprehensive ATLAS aQGC EFT constraints to date and is competitive with the corresponding CMS combinations. The transparent construction of the joint likelihood (documented overlap removal, fully correlated experimental systematics, validated Wilks’ theorem within 5 %), the systematic treatment of unitarization via clipping, and the inclusion of profiled multi-operator fits make the results immediately usable for phenomenological reinterpretation. The quantification of template-replacement non-closure (percent-level) further increases confidence in the coverage of the full operator set.

minor comments (5)
  1. [§3] §3: The decision not to include the quantified template-replacement non-closure (up to 9 % on f_M1 and f_T9, widening intervals by at most 4 %) as a systematic uncertainty in the final results should be stated more prominently, ideally with a short sentence in the caption of Table 2 or Figure 2.
  2. [Table 1, §2] Table 1 and §2: The exclusion of O_T3 and O_T4 is attributed solely to the unavailability of MadGraph implementations in the original publications; a one-sentence remark on whether these operators are expected to be redundant or weakly constrained by the present data set would help the reader.
  3. [Figures 2–3] Figure 2 (bottom panel) and Figure 3: The two illustrative values f = 1 and f = (4π)^2 used for the Λ reach are not defined in the text; a brief parenthetical explanation would improve readability.
  4. [§4] §4: The statement that “the choice of correlation scheme ho has negligible impact ho changing by less than one percent” is useful; adding the extreme case (all systematics uncorrelated) as a parenthetical would make the claim fully self-contained.
  5. Throughout: Occasional typographic artefacts remain (e.g., “ORGANISA TION”, “Éboli” inconsistently accented, missing spaces around some equation numbers). A final proof-reading pass is recommended.

Circularity Check

0 steps flagged

No significant circularity: standard joint-likelihood combination of independent ATLAS measurements constraining free EFT Wilson coefficients.

full rationale

The paper constructs a joint likelihood from seven published VBS analyses and one triboson analysis (Table 1), treats the 17 Éboli Wilson coefficients as free parameters of interest, and extracts 68%/95% CL intervals (one- and two-dimensional, profiled, unitarized via clipping) via standard profile-likelihood fits (Eq. 3, Wilks). SM and EFT matrix elements are taken from external generators (MadGraph5_aMC@NLO + Pythia) and theory references (Éboli model, unitarity bounds of Refs. [37,38], positivity of Ref. [39]); no coefficient is defined in terms of another fitted quantity, no fitted parameter is re-labeled a prediction, and no uniqueness theorem or ansatz is imported from overlapping authors to force the result. Self-citations are solely to the input ATLAS measurements whose data are re-used—an ordinary and transparent feature of combination papers—and do not load-bear any theoretical claim. Minor technical choices (template replacement, omission of OT3/OT4) are quantified at the percent level and do not create definitional loops. The derivation is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 5 axioms · 0 invented entities

The central claim rests on the validity of the dimension-8 EFT truncation, the completeness of the Éboli operator basis after removing redundancies, the negligibility of residual dimension-6 effects, the correctness of the MadGraph+Pythia simulation chain, and the external unitarity and positivity bounds. No new particles or forces are postulated; the Wilson coefficients themselves are the free parameters of interest being constrained by data.

free parameters (1)
  • 17 Wilson coefficients f_i/Λ⁴ (Éboli basis) = see Tables 2–3 and Figs. 2–5
    These are the parameters of interest floated in the likelihood fits; their fitted intervals constitute the result. They are not fixed by hand but are free within the EFT.
axioms (5)
  • domain assumption Dimension-6 operators that generate anomalous triple-gauge couplings are already sufficiently constrained that their contribution to the analyzed VBS and triboson channels can be neglected.
    Stated explicitly in the Introduction and §2; if false the extracted dim-8 intervals are biased.
  • domain assumption The Éboli basis (after dropping O_M6, O_T3, O_T4 and identifying f_S0 = f_S2) spans the relevant C-even P-even dimension-8 aQGC operators.
    Adopted from Refs. [8,36]; used throughout the simulation and fit.
  • domain assumption Perturbative partial-wave unitarity bounds of Refs. [37,38] and positivity bounds of Ref. [39] correctly delimit the EFT validity region.
    Used to define the unitarization cut-off via the clipping procedure (§5).
  • standard math Wilks’ theorem holds for the profile-likelihood ratio, so that 68 %/95 % CL intervals can be read from ΔNLL = 1/3.84 (1 dof) or the corresponding 2-dof contours.
    Validated against pseudo-experiments to within 5 % (§4).
  • domain assumption MadGraph5_aMC@NLO + MadSpin + Pythia 8 (dipole recoil) correctly generates the linear, quadratic and cross-term EFT contributions at LO QCD.
    Simulation setup of §2; higher-order SM samples from the original analyses are retained for the SM piece.

pith-pipeline@v1.1.0-grok45 · 52575 in / 2835 out tokens · 28193 ms · 2026-07-15T11:53:33.775831+00:00 · methodology

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read the original abstract

A combination of measurements sensitive to anomalous quartic electroweak gauge boson couplings is presented using proton-proton collision data collected by the ATLAS detector at $\sqrt{s} = 13$ TeV at the LHC. Contributing analyses include measurements of vector-boson scattering in numerous final states as well as a tri-boson measurement. The combined measurement is used to constrain anomalous electroweak boson quartic self-couplings that result from dimension-8 operators in the \'{E}boli model using an effective field theory. Results are presented as 68% and 95% confidence level intervals parameterised by one or two Wilson coefficients, both with and without unitarity constraints applied. Theoretical bounds from unitarity and positivity are overlaid where relevant. Confidence intervals obtained from simultaneous profiled fits to all Wilson coefficients are also presented.

discussion (0)

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Reference graph

Works this paper leans on

48 extracted references · 43 linked inside Pith

  1. [1]

    ATLAS Collaboration,Combination of searches for heavy spin-1 resonances using139fb−1 of proton–proton collision data at√𝑠=13TeV with the ATLAS detector, JHEP04(2024) 118, arXiv:2402.10607 [hep-ex]

  2. [2]

    CMS Collaboration, Combination of CMS searches for heavy resonances decaying to pairs of bosons or leptons, Phys. Lett. B798(2019) 134952, arXiv:1906.00057 [hep-ex]

  3. [3]

    Brivio and M

    I. Brivio and M. Trott,The standard model as an effective field theory, Phys. Rept.793(2019) 1, arXiv:1706.08945 [hep-ph]. 14

  4. [4]

    ATLAS Collaboration,Interpretations of the ATLAS measurements of Higgs boson production and decay rates and differential cross-sections in𝑝 𝑝collisions at√𝑠=13TeV, JHEP11(2024) 097, arXiv:2402.05742 [hep-ex]

  5. [5]

    CMS Collaboration,Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements, (2025), arXiv:2504.02958 [hep-ex]

  6. [6]

    Rept.427(2006) 257, arXiv:hep-ex/0509008

    ALEPH Collaboration, DELPHI Collaboration, L3 Collaboration, OPAL Collaboration, SLD Collaboration, LEP Electroweak Working Group, and SLD electroweak and heavy flavour groups, Precision electroweak measurements on the Z resonance, Phys. Rept.427(2006) 257, arXiv:hep-ex/0509008

  7. [7]

    O. J. P. Éboli, M. C. Gonzalez-Garcia and S. Lietti,Bosonic quartic couplings at CERN LHC, Phys. Rev. D69(2004) 095005, arXiv:hep-ph/0310141

  8. [8]

    O. J. Éboli, M. Gonzalez-Garcia and J. Mizukoshi,𝑝 𝑝→𝑗 𝑗 𝑒±𝜇±𝜈𝜈and𝑗 𝑗 𝑒 ±𝜇∓𝜈𝜈at𝑂(𝛼 6 𝑒𝑚) and𝑂(𝛼 4 𝑒𝑚𝛼2 𝑠)for the study of the quartic electroweak gauge boson vertex at CERN LHC, Phys. Rev. D74(2006) 073005, arXiv:hep-ph/0606118

  9. [9]

    Contino, D

    R. Contino, D. Pappadopulo, D. Marzocca and R. Rattazzi, On the effect of resonances in composite Higgs phenomenology, JHEP10(2011) 081, arXiv:1109.1570 [hep-ph]

  10. [10]

    Randall and R

    L. Randall and R. Sundrum,Large mass hierarchy from a small extra dimension, Phys. Rev. Lett.83(1999) 3370, arXiv:hep-ph/9905221

  11. [11]

    Agashe, H

    K. Agashe, H. Davoudiasl, G. Perez and A. Soni,Warped gravitons at the CERN LHC and beyond, Phys. Rev. D76(2007) 036006, arXiv:hep-ph/0701186

  12. [12]

    G. C. Branco et al.,Theory and phenomenology of two-Higgs-doublet models, Phys. Rept.516(2012) 1, arXiv:1106.0034 [hep-ph]

  13. [13]

    Georgi and S

    H. Georgi and S. L. Glashow,Unity of all elementary-particle forces, Phys. Rev. Lett.32(1974) 438

  14. [14]

    ATLAS Collaboration,Measurement and interpretation of same-sign𝑊boson pair production in association with two jets in𝑝 𝑝collisions at√𝑠=13TeV with the ATLAS detector, JHEP04(2024) 026, arXiv:2312.00420 [hep-ex]

  15. [15]

    CMS Collaboration,Observation of Electroweak Production of Same-Sign𝑊Boson Pairs in the Two Jet and Two Same-Sign Lepton Final State in Proton–Proton Collisions at√𝑠=13TeV, Phys. Rev. Lett.120(2018) 081801, arXiv:1709.05822 [hep-ex]

  16. [16]

    ATLAS Collaboration,Observation of electroweak production of𝑊 +𝑊 − in association with jets in proton–proton collisions at√𝑠=13TeV with the ATLAS Detector, JHEP07(2024) 254, arXiv:2403.04869 [hep-ex]

  17. [17]

    CMS Collaboration,Observation of electroweak𝑊 +𝑊 − pair production in association with two jets in proton–proton collisions at√𝑠=13TeV, Phys. Lett. B841(2023) 137495, arXiv:2205.05711 [hep-ex]

  18. [18]

    ATLAS Collaboration,Measurements of electroweak𝑊 ±𝑍boson pair production in association with two jets in𝑝 𝑝collisions at√𝑠=13TeV with the ATLAS detector, JHEP06(2024) 192, arXiv:2403.15296 [hep-ex]

  19. [19]

    CMS Collaboration,Measurement of electroweak𝑊 𝑍 boson production and search for new physics in𝑊 𝑍+two jets events in𝑝 𝑝collisions at √𝑠=13TeV, Phys. Lett. B795(2019) 281, arXiv:1901.04060 [hep-ex]. 15

  20. [20]

    ATLAS Collaboration,Differential cross-section measurements of the production of four charged leptons in association with two jets using the ATLAS detector, JHEP01(2024) 004, arXiv:2308.12324 [hep-ex]

  21. [21]

    CMS Collaboration,Evidence for electroweak production of four charged leptons and two jets in proton–proton collisions at√𝑠=13TeV, Phys. Lett. B812(2021) 135992, arXiv:2008.07013 [hep-ex]

  22. [22]

    ATLAS Collaboration,Fiducial and differential cross-section measurements of electroweak𝑊 𝛾 𝑗 𝑗 production in𝑝 𝑝collisions at √𝑠=13TeV with the ATLAS detector, Eur. Phys. J. C84(2024) 1064, arXiv:2403.02809 [hep-ex]

  23. [23]

    CMS Collaboration,Measurement of the electroweak production of𝑊 𝛾in association with two jets in proton–proton collisions at√𝑠=13TeV, Phys. Rev. D108(2023) 032017, arXiv:2212.12592 [hep-ex]

  24. [24]

    ATLAS Collaboration,Measurement of electroweak𝑍(𝜈¯𝜈)𝛾 𝑗 𝑗production and limits on anomalous quartic gauge couplings in𝑝 𝑝collisions at√𝑠=13TeV with the ATLAS detector, JHEP06(2023) 082, arXiv:2208.12741 [hep-ex]

  25. [25]

    ATLAS Collaboration,Measurement of the cross-sections of the electroweak and total production of a𝑍 𝛾pair in association with two jets in𝑝 𝑝collisions at√𝑠=13TeV with the ATLAS detector, Phys. Lett. B846(2023) 138222, arXiv:2305.19142 [hep-ex]

  26. [26]

    CMS Collaboration,Measurement of the electroweak production of𝑍 𝛾and two jets in proton–proton collisions at√𝑠=13TeV and constraints on anomalous quartic gauge couplings, Phys. Rev. D104(2021) 072001, arXiv:2106.11082 [hep-ex]

  27. [27]

    ATLAS Collaboration,Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from𝑝 𝑝collisions at√𝑠=13TeV with the ATLAS detector, (2025), arXiv:2503.17461 [hep-ex]

  28. [28]

    CMS Collaboration,Evidence for𝑊𝑊/𝑊 𝑍vector boson scattering in the decay channelℓ𝜈𝑞𝑞 produced in association with two jets in proton–proton collisions at√𝑠=13TeV, Phys. Lett. B834(2022) 137438, arXiv:2112.05259 [hep-ex]

  29. [29]

    ATLAS Collaboration,Observation of𝑊 𝛾𝛾triboson production in proton–proton collisions at√𝑠=13TeV with the ATLAS detector, Phys. Lett. B848(2024) 138400, arXiv:2308.03041 [hep-ex]

  30. [30]

    ATLAS Collaboration, Observation of𝑊𝑊𝑊Production in𝑝 𝑝Collisions at √𝑠=13TeV with the ATLAS Detector, Phys. Rev. Lett.129(2022) 061803, arXiv:2201.13045 [hep-ex]

  31. [31]

    ATLAS Collaboration,Observation of𝑉𝑉 𝑍production at √𝑠=13TeV with the ATLAS detector, Phys. Lett. B866(2025) 139527, arXiv:2412.15123 [hep-ex]

  32. [32]

    CMS Collaboration,Observation of the production of three massive gauge bosons at√𝑠=13TeV, Phys. Rev. Lett.125(2020) 151802, arXiv:2006.11191 [hep-ex]

  33. [33]

    CMS Collaboration,Measurements of the𝑝 𝑝→𝑊 ±𝛾𝛾and𝑝 𝑝→𝑍 𝛾𝛾cross sections at√𝑠=13TeV and limits on anomalous quartic gauge couplings, JHEP10(2021) 174, arXiv:2105.12780 [hep-ex]

  34. [34]

    CMS Collaboration,Observation of𝑊𝑊 𝛾Production and Search for𝐻𝛾Production in Proton–Proton Collisions at√𝑠=13TeV, Phys. Rev. Lett.132(2024) 121901, arXiv:2310.05164 [hep-ex]. 16

  35. [35]

    CMS Collaboration,Observation of𝑊 𝑍 𝛾production and constraints on new physics scenarios in proton–proton collisions at√𝑠=13TeV, Phys. Rev. D112(2025) 012009, arXiv:2503.21977 [hep-ex]

  36. [36]

    O. J. P. Éboli and M. Gonzalez-Garcia,Mapping the genuine bosonic quartic couplings, Phys. Rev. D93(2016) 093013, arXiv:1604.03555 [hep-ph]

  37. [37]

    E. d. S. Almeida, O. J. P. Éboli and M. C. Gonzalez–Garcia, Unitarity constraints on anomalous quartic couplings, Phys. Rev. D101(2020) 113003, arXiv:2004.05174 [hep-ph]

  38. [38]

    O. J. P. Éboli and M. C. Gonzalez–Garcia,Unitarity limits on triple gauge boson production, (2026), arXiv:2601.07920 [hep-ph]

  39. [39]

    G. N. Remmen and N. L. Rodd,Consistency of the standard model effective field theory, JHEP12(2019) 32, arXiv:1908.09845 [hep-ph]

  40. [40]

    J. Alwall 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, arXiv:1405.0301 [hep-ph]

  41. [41]

    NNPDF Collaboration, R. D. Ball et al.,Parton distributions for the LHC run II, JHEP04(2015) 040, arXiv:1410.8849 [hep-ph]

  42. [42]

    Artoisenet, R

    P. Artoisenet, R. Frederix, O. Mattelaer and R. Rietkerk, Automatic spin-entangled decays of heavy resonances in Monte Carlo simulations, JHEP03(2013) 015, arXiv:1212.3460 [hep-ph]

  43. [43]

    Sjöstrand et al.,An introduction to PYTHIA 8.2, Comput

    T. Sjöstrand et al.,An introduction to PYTHIA 8.2, Comput. Phys. Commun.191(2015) 159, arXiv:1410.3012 [hep-ph]

  44. [44]

    Cowan, K

    G. Cowan, K. Cranmer, E. Gross and O. Vitells, Asymptotic formulae for likelihood-based tests of new physics, Eur. Phys. J. C71(2011) 1554, arXiv:1007.1727 [physics.data-an], Erratum: Eur. Phys. J. C73(2013) 2501

  45. [45]

    CMS Collaboration,Measurements of production cross sections of𝑊 𝑍and same-sign𝑊𝑊boson pairs in association with two jets in proton–proton collisions at√𝑠=13TeV, Phys. Lett. B809(2020) 135710, arXiv:2005.01173 [hep-ex]

  46. [46]

    CMS Collaboration,Vector boson scattering and anomalous quartic couplings in final states with ℓ𝜈𝑞𝑞orℓℓ𝑞𝑞plus jets using proton–proton collisions at√𝑠=13TeV, (2025), arXiv:2510.00118 [hep-ex]

  47. [47]

    CMS Collaboration,Search for high-mass exclusive𝛾𝛾→𝑊𝑊and𝛾𝛾→𝑍 𝑍production in proton–proton collisions at√𝑠=13TeV, JHEP07(2023) 229, arXiv:2211.16320 [hep-ex]

  48. [48]

    Demokritos

    ATLAS Collaboration,ATLAS Computing Acknowledgements, ATL-SOFT-PUB-2026-001, 2026, url:https://cds.cern.ch/record/2952666. 17 The ATLAS Collaboration G. Aad 102, E. Aakvaag 17, B. Abbott 122, S. Abdelhameed 118a, K. Abeling 54, N.J. Abicht 48, S.H. Abidi 30, M. Aboelela 44, A. Aboulhorma 36e, H. Abramowicz 155, B.S. Acharya 68a,68b,m, A. Ackermann 62a, C....