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arxiv: 2605.15396 · v1 · pith:7FA67I22new · submitted 2026-05-14 · ✦ hep-ex

First measurements of vector boson scattering in W^pmW^{pm} and WZ production in all-leptonic final states at sqrt{s} = 13.6 TeV

Pith reviewed 2026-05-19 15:06 UTC · model grok-4.3

classification ✦ hep-ex
keywords vector boson scatteringelectroweak productionW±W±WZCMS13.6 TeVleptonic final statesproton-proton collisions
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The pith

Electroweak production of W±W± and WZ pairs with two jets observed at over five sigma each in leptonic decays.

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

This paper reports measurements of the production cross sections for W±W± and WZ boson pairs produced in association with two jets in proton-proton collisions at 13.6 TeV. The analysis uses 171 fb^{-1} of data collected by the CMS detector and focuses on the fully leptonic final states where both bosons decay to electrons or muons. The electroweak components of these processes are extracted and shown to exceed five standard deviations above background-only expectations. Differential fiducial cross sections are measured as functions of several kinematic observables. These results directly probe the vector boson scattering mechanism predicted by the Standard Model at the new collision energy.

Core claim

The electroweak productions of W±W± and WZ bosons are each observed with a significance greater than five standard deviations from the background-only hypothesis in the leptonic decay modes W±Z → ℓ±νℓ′±ℓ′∓ and W±W± → ℓ±νℓ′±ν at √s = 13.6 TeV with an integrated luminosity of 171 fb^{-1}.

What carries the argument

Electroweak production of diboson pairs with two jets, isolated in all-leptonic final states to extract the vector boson scattering contribution.

If this is right

  • The measured cross sections test the Standard Model prediction for vector boson scattering at the highest proton collision energy recorded so far.
  • Differential distributions provide constraints on possible anomalous quartic gauge couplings.
  • The results establish a reference for searches for deviations from the Standard Model in high-energy diboson final states.
  • The all-leptonic channels offer a clean signature for future precision studies of electroweak interactions.

Where Pith is reading between the lines

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

  • Extending the same selection to higher integrated luminosities could reveal subtle kinematic deviations that hint at new physics.
  • Combining these leptonic measurements with semi-leptonic or fully hadronic channels may improve limits on effective field theory operators.
  • The techniques developed here for background subtraction in high-pileup environments can be applied to other rare electroweak processes at the LHC.
  • If future data show tension in specific angular or mass distributions, it would point to modifications in the longitudinal scattering amplitude.

Load-bearing premise

Background processes in the selected leptonic final states are accurately estimated by a combination of Monte Carlo simulation and data-driven methods without significant mismodeling that could mimic the electroweak signal.

What would settle it

A revision of the data-driven background estimates in the signal regions that increases the predicted background yield enough to drop either observed significance below five standard deviations.

Figures

Figures reproduced from arXiv: 2605.15396 by CMS Collaboration.

Figure 1
Figure 1. Figure 1: Representative Feynman diagrams of a VBS process contributing to the EW-induced [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Representative Feynman diagrams of the QCD-induced production of W [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Distributions of mjj (upper left), mℓℓ (upper right), ∆ηjj (center left), ∆ϕjj (center right), and nj (lower) in the W±W± SR. The predicted yields are shown with their best fit normaliza￾tions from the simultaneous fit. Vertical bars on data points represent the statistical uncertainty in the data. The histograms for tVx backgrounds include the contributions from ttV and tZq processes. The histograms for t… view at source ↗
Figure 4
Figure 4. Figure 4: Distributions of the BDT score (left) and [PITH_FULL_IMAGE:figures/full_fig_p013_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Measured and predicted absolute EW W±W± cross sections in bins of mjj (upper left), mℓℓ (upper right), ∆ηjj (center left), ∆ϕjj (center right), and nj (lower). The ratios of the predictions to the data are also shown. The measurements are compared with the predic￾tions from the MADGRAPH5 aMC@NLO and SHERPA generators. The shaded bands and un￾certainty bars around the data points correspond to the total mea… view at source ↗
Figure 6
Figure 6. Figure 6: Measured and predicted normalized EW W±W± cross sections in bins of mjj (up￾per left), mℓℓ (upper right), ∆ηjj (center left), ∆ϕjj (center right), and nj (lower). The ratios of the predictions to the data are also shown. The measurements are compared with the pre￾dictions from the MADGRAPH5 aMC@NLO and SHERPA generators. The shaded bands and uncertainty bars around the data points correspond to the total m… view at source ↗
Figure 7
Figure 7. Figure 7: Measured and predicted absolute (left) and normalized (right) EW WZ cross sections [PITH_FULL_IMAGE:figures/full_fig_p018_7.png] view at source ↗
read the original abstract

The production cross sections of W$^\pm$W$^{\pm}$ and WZ boson pairs in association with two jets in proton-proton collisions are measured at $\sqrt{s}$ = 13.6 TeV. The data sample corresponds to an integrated luminosity of 171 fb$^{-1}$, collected with the CMS detector during 2022$-$2024. The measurements are performed in the leptonic decay modes: W$^{\pm}$Z $\to$ $\ell^\pm\nu\ell^{\prime\pm}\ell^{\prime\mp}$ and W$^\pm$W$^{\pm}$ $\to$ $\ell^\pm\nu\ell^{\prime\pm}\nu$, where $\ell, \ell'$ = e or $\mu$. The electroweak productions of W$^\pm$W$^{\pm}$ and WZ bosons are each observed with a significance greater than five standard deviations from the background-only hypothesis. Differential fiducial cross sections as functions of several observables are also measured.

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 manuscript reports first measurements of vector boson scattering (VBS) in the electroweak production of W±W± and WZ boson pairs in association with two jets, using the all-leptonic final states at √s = 13.6 TeV with the CMS detector. The data correspond to 171 fb⁻¹ collected in 2022–2024. The analysis extracts fiducial cross sections and observes both EW W±W± and WZ processes with significances greater than 5σ above the background-only hypothesis. Differential fiducial cross sections as functions of several observables are also presented.

Significance. If the background modeling and systematic uncertainties are robustly validated, this constitutes an important extension of prior VBS measurements to the new center-of-mass energy and integrated luminosity. The all-leptonic channels provide a clean experimental signature, and the reported observations would strengthen constraints on electroweak gauge couplings and serve as a baseline for future anomalous quartic gauge coupling searches.

major comments (1)
  1. [Background estimation and systematic uncertainties] Background estimation section: The central >5σ significance claims for both EW W±W± and WZ rest on the accuracy of the combined MC + data-driven background model (tt̄, non-prompt leptons, Z+jets, charge-flip) after the two-jet VBS selection. The manuscript should include explicit closure tests or high-statistics validation plots in control regions with jet multiplicity, pT balance, and mjj distributions matching the signal-enriched phase space to demonstrate that residual mismodeling does not bias the fitted signal strength or inflate the observed significance. Without such tests, the background-only hypothesis rejection remains vulnerable to the concern raised in the stress-test note.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful and constructive review of our manuscript reporting the first measurements of electroweak W±W± and WZ production with two jets in the all-leptonic final states at 13.6 TeV. We appreciate the emphasis placed on the robustness of the background modeling, which underpins the significance of the observations. Below we respond point by point to the major comment and outline the revisions we will make.

read point-by-point responses
  1. Referee: Background estimation section: The central >5σ significance claims for both EW W±W± and WZ rest on the accuracy of the combined MC + data-driven background model (tt̄, non-prompt leptons, Z+jets, charge-flip) after the two-jet VBS selection. The manuscript should include explicit closure tests or high-statistics validation plots in control regions with jet multiplicity, pT balance, and mjj distributions matching the signal-enriched phase space to demonstrate that residual mismodeling does not bias the fitted signal strength or inflate the observed significance. Without such tests, the background-only hypothesis rejection remains vulnerable to the concern raised in the stress-test note.

    Authors: We agree that explicit validation of the background model is important for supporting the reported significances. The manuscript already describes a hybrid background estimation that combines Monte Carlo predictions for tt̄, Z+jets and other processes with data-driven estimates for non-prompt leptons and charge-flip backgrounds. Control regions with relaxed VBS selections (lower mjj, altered jet multiplicity) are used to constrain and validate the modeling, and these are incorporated into the simultaneous fit for the signal strengths. The systematic uncertainties assigned to the background components are designed to cover residual mismodeling. To directly address the referee’s request, we will add dedicated closure tests and high-statistics validation plots in the revised manuscript. These will show data-to-prediction comparisons for jet multiplicity, vector-boson pT balance, and mjj distributions in control regions whose kinematics closely match the signal-enriched phase space. We believe these additions will demonstrate that any residual discrepancies do not bias the fitted signal strengths or inflate the observed significances beyond the quoted uncertainties. With respect to the stress-test note, the current uncertainty model already includes variations that probe the relevant modeling assumptions; the new plots will provide further transparency. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected in experimental observation claim

full rationale

The paper presents a direct experimental measurement of electroweak VBS cross sections and observation significances extracted from 171 fb^{-1} of 13.6 TeV collision data in all-leptonic final states. The central result is a statistical excess over a background-only hypothesis, with backgrounds estimated via a combination of Monte Carlo simulation and data-driven techniques. No derivation chain reduces by the paper's own equations or self-citations to quantities defined solely by fitted parameters; the reported >5σ significances and differential cross sections are data-driven quantities whose validity rests on external validation of the background model rather than internal self-definition or renaming of inputs as predictions. The analysis is self-contained against external benchmarks and does not invoke load-bearing uniqueness theorems or ansatzes from prior author work.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The observation claim rests on standard high-energy physics assumptions for background modeling and detector response rather than new postulates or free parameters introduced in this work.

axioms (2)
  • domain assumption The Standard Model accurately describes the dominant background processes in the all-leptonic final states with two jets.
    Required to define the background-only hypothesis against which the >5σ excess is measured.
  • domain assumption Lepton and jet reconstruction efficiencies and resolutions are correctly modeled in simulation.
    Necessary to convert observed event yields into fiducial cross sections.

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Reference graph

Works this paper leans on

88 extracted references · 88 canonical work pages · 50 internal anchors

  1. [1]

    Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC

    ATLAS Collaboration, “Observation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHC”,Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214

  2. [2]

    Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC

    CMS Collaboration, “Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC”,Phys. Lett. B716(2012) 30, doi:10.1016/j.physletb.2012.08.021,arXiv:1207.7235

  3. [3]

    Observation of a new boson with mass near 125 GeV in pp collisions at sqrt(s) = 7 and 8 TeV

    CMS Collaboration, “Observation of a new boson with mass near 125 GeV in pp collisions at √s= 7 and 8 TeV”,JHEP06(2013) 081, doi:10.1007/JHEP06(2013)081,arXiv:1303.4571

  4. [4]

    Broken symmetry and the mass of gauge vector mesons

    F. Englert and R. Brout, “Broken symmetry and the mass of gauge vector mesons”,Phys. Rev. Lett.13(1964) 321,doi:10.1103/PhysRevLett.13.321

  5. [5]

    Broken symmetries, massless particles and gauge fields

    P . W. Higgs, “Broken symmetries, massless particles and gauge fields”,Phys. Lett.12 (1964) 132,doi:10.1016/0031-9163(64)91136-9

  6. [6]

    Broken symmetries and the masses of gauge bosons

    P . W. Higgs, “Broken symmetries and the masses of gauge bosons”,Phys. Rev. Lett.13 (1964) 508,doi:10.1103/PhysRevLett.13.508

  7. [7]

    Global conservation laws and massless particles

    G. S. Guralnik, C. R. Hagen, and T. W. B. Kibble, “Global conservation laws and massless particles”,Phys. Rev. Lett.13(1964) 585,doi:10.1103/PhysRevLett.13.585

  8. [8]

    Spontaneous symmetry breakdown without massless bosons

    P . W. Higgs, “Spontaneous symmetry breakdown without massless bosons”,Phys. Rev. 145(1966) 1156,doi:10.1103/PhysRev.145.1156. 18

  9. [9]

    Symmetry breaking in non-Abelian gauge theories

    T. W. B. Kibble, “Symmetry breaking in non-Abelian gauge theories”,Phys. Rev.155 (1967) 1554,doi:10.1103/PhysRev.155.1554

  10. [10]

    Longitudinal WW scattering in light of the "Higgs" discovery

    D. Espriu and B. Yencho, “Longitudinal WW scattering in light of the Higgs boson discovery”,Phys. Rev. D87(2013) 055017,doi:10.1103/PhysRevD.87.055017, arXiv:1212.4158

  11. [11]

    WW Scattering in the Era of Post Higgs Discovery

    J. Chang, K. Cheung, C.-T. Lu, and T.-C. Yuan, “WW scattering in the era of post-Higgs-boson discovery”,Phys. Rev. D87(2013) 093005, doi:10.1103/PhysRevD.87.093005,arXiv:1303.6335

  12. [12]

    Strength of weak interactions at very high-energies and the Higgs boson mass

    B. W. Lee, C. Quigg, and H. B. Thacker, “Strength of weak interactions at very high-energies and the Higgs boson mass”,Phys. Rev. Lett.38(1977) 883, doi:10.1103/PhysRevLett.38.883

  13. [13]

    Weak interactions at very high energies: the role of the Higgs boson mas

    B. W. Lee, C. Quigg, and H. B. Thacker, “Weak interactions at very high energies: the role of the Higgs boson mas”,Phys. Rev. D16(1977) 1519, doi:10.1103/PhysRevD.16.1519

  14. [14]

    p p -> j j e+/- mu+/- nu nu and j j e+/- mu-/+ nu nu at O(\alpha_{em}^6) and O(\alpha_{em}^4 \alpha_s^2) for the Study of the Quartic Electroweak Gauge Boson Vertex at LHC

    O. J. P . ´Eboli, M. C. Gonzalez-Garcia, and J. K. Mizukoshi, “pp→jje ±µ±ννand jje ±µ∓νν atO(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,doi:10.1103/PhysRevD.74.073005, arXiv:hep-ph/0606118

  15. [15]

    Same-sign WW Scattering in the HEFT: Discoverability vs. EFT Validity

    P . Koz´ow, L. Merlo, S. Pokorski, and M. Szleper, “Same-sign WW scattering in the HEFT: discoverability vs. EFT validity”,JHEP07(2019) 021, doi:10.1007/JHEP07(2019)021,arXiv:1905.03354

  16. [16]

    Same-sign WW scattering at the LHC: can we discover BSM effects before discovering new states?

    J. Kalinowski et al., “Same-sign WW scattering at the LHC: can we discover BSM effects before discovering new states?”,Eur. Phys. J. C78(2018) 403, doi:10.1140/epjc/s10052-018-5885-y,arXiv:1802.02366

  17. [17]

    A sensitivity study of VBS and diboson WW to dimension-6 EFT operators at the LHC

    R. Bellan et al., “A sensitivity study of VBS and diboson WW to dimension-6 EFT operators at the LHC”,JHEP05(2022) 039,doi:10.1007/JHEP05(2022)039, arXiv:2108.03199

  18. [18]

    SMEFT analysis of vector boson scattering and diboson data from the LHC run II

    J. J. Ethier, R. Gomez-Ambrosio, G. Magni, and J. Rojo, “SMEFT analysis of vector boson scattering and diboson data from the LHC run II”,Eur. Phys. J. C81(2021) 560, doi:10.1140/epjc/s10052-021-09347-7,arXiv:2101.03180

  19. [19]

    Standard model EFT effects in vector-boson scattering at the LHC

    A. Dedes, P . Koz´ow, and M. Szleper, “Standard model EFT effects in vector-boson scattering at the LHC”,Phys. Rev. D104(2021) 013003, doi:10.1103/PhysRevD.104.013003,arXiv:2011.07367

  20. [20]

    Majorana neutrinos in same-signW ±W± scattering at the LHC: Breaking the TeV barrier

    B. Fuks et al., “Majorana neutrinos in same-signW ±W± scattering at the LHC: Breaking the TeV barrier”,Phys. Rev. D103(2021) 055005, doi:10.1103/PhysRevD.103.055005,arXiv:2011.02547

  21. [21]

    Study of vector boson scattering and search for new physics in events with two same-sign leptons and two jets

    CMS Collaboration, “Study of vector boson scattering and search for new physics in events with two same-sign leptons and two jet”,Phys. Rev. Lett.114(2015) 051801, doi:10.1103/PhysRevLett.114.051801,arXiv:1410.6315

  22. [22]

    Evidence for Electroweak Production of $W^{\pm}W^{\pm}jj$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

    ATLAS Collaboration, “Evidence for electroweak production ofW ±W±jj in pp collisions at √s= 8 TeV with the ATLAS detector”,Phys. Rev. Lett.113(2014) 141803, doi:10.1103/PhysRevLett.113.141803,arXiv:1405.6241. References 19

  23. [23]

    Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV

    CMS Collaboration, “Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at √s= 13 TeV”,Phys. Rev. Lett.120(2018) 081801,doi:10.1103/PhysRevLett.120.081801, arXiv:1709.05822

  24. [24]

    Observation of electroweak production of a same-sign W boson pair in association with two jets in pp collisions at √s=13 TeV with the ATLAS detector

    ATLAS Collaboration, “Observation of electroweak production of a same-sign W boson pair in association with two jets in pp collisions at √s=13 TeV with the ATLAS detector”,Phys. Rev. Lett.123(2019) 161801, doi:10.1103/PhysRevLett.123.161801,arXiv:1906.03203

  25. [25]

    Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at √s=13 TeV with the atlas detector

    ATLAS Collaboration, “Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at √s=13 TeV with the atlas detector”,JHEP04(2024) 026,doi:10.1007/JHEP04(2024)026, arXiv:2312.00420

  26. [26]

    Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets in proton-proton collisions at √s= 13 TeV

    CMS Collaboration, “Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets in proton-proton collisions at √s= 13 TeV”, Phys. Lett. B809(2020) 135710,doi:10.1016/j.physletb.2020.135710, arXiv:2005.01173

  27. [27]

    Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on anomalous gauge boson self-couplings

    ATLAS Collaboration, “Measurements of W ±Z production cross sections in pp collisions at √s=8 TeV with the ATLAS detector and limits on anomalous gauge boson self-couplings”,Phys. Rev. D93(2016) 092004,doi:10.1103/PhysRevD.93.092004, arXiv:1603.02151

  28. [28]

    Measurement of electroweak WZ boson production and search for new physics in WZ $+$ two jets events in pp collisions at $\sqrt{s} =$ 13 TeV

    CMS Collaboration, “Measurement of electroweak WZ boson production and search for new physics in WZ + two jets events in pp collisions at √s= 13 TeV”,Phys. Lett. B795 (2019) 281,doi:10.1016/j.physletb.2019.05.042,arXiv:1901.04060

  29. [29]

    Observation of electroweak $W^{\pm}Z$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

    ATLAS Collaboration, “Observation of electroweakW ±Zboson pair production in association with two jets in pp collisions at √s= 13 TeV with the ATLAS detector”,Phys. Lett. B793(2019) 469,doi:10.1016/j.physletb.2019.05.012, arXiv:1812.09740

  30. [30]

    Measurements of electroweak W ±Z boson pair production in association with two jets in pp collisions at √s= 13 TeV with the atlas detector

    ATLAS Collaboration, “Measurements of electroweak W ±Z boson pair production in association with two jets in pp collisions at √s= 13 TeV with the atlas detector”,JHEP 06(2024) 192,doi:10.1007/JHEP06(2024)192,arXiv:2403.15296

  31. [31]

    HEPData record for this analysis

    “HEPData record for this analysis”, 2026.doi:10.17182/hepdata.169760

  32. [32]

    The CMS experiment at the CERN LHC

    CMS Collaboration, “The CMS experiment at the CERN LHC”,JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004

  33. [33]

    Development of the CMS detector for the CERN LHC Run 3

    CMS Collaboration, “Development of the CMS detector for the CERN LHC Run 3”, JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064

  34. [34]

    Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV

    CMS Collaboration, “Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV”,JINST15(2020) P10017,doi:10.1088/1748-0221/15/10/P10017, arXiv:2006.10165

  35. [35]

    The CMS trigger system

    CMS Collaboration, “The CMS trigger system”,JINST12(2017) P01020, doi:10.1088/1748-0221/12/01/P01020,arXiv:1609.02366. 20

  36. [36]

    Performance of the CMS high-level trigger during LHC run 2

    CMS Collaboration, “Performance of the CMS high-level trigger during LHC Run 2”, JINST19(2024) P11021,doi:10.1088/1748-0221/19/11/P11021, arXiv:2410.17038

  37. [37]

    Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC

    CMS Collaboration, “Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC”,JINST16(2021) P05014, doi:10.1088/1748-0221/16/05/P05014,arXiv:2012.06888

  38. [38]

    Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\sqrt{s}=$ 13 TeV

    CMS Collaboration, “Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s=13 TeV”,JINST13(2018) P06015, doi:10.1088/1748-0221/13/06/P06015,arXiv:1804.04528

  39. [39]

    Description and performance of track and primary-vertex reconstruction with the CMS tracker

    CMS Collaboration, “Description and performance of track and primary-vertex reconstruction with the CMS tracker”,JINST9(2014) P10009, doi:10.1088/1748-0221/9/10/P10009,arXiv:1405.6569

  40. [40]

    The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations

    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,doi:10.1007/JHEP07(2014)079,arXiv:1405.0301

  41. [41]

    MadGraph 5 : Going Beyond

    J. Alwall et al., “Madgraph 5: going beyond”,JHEP06(2011) 128, doi:10.1007/JHEP06(2011)128,arXiv:1106.0522

  42. [42]

    Merging meets matching in MC@NLO

    R. Frederix and S. Frixione, “Merging meets matching in MC@NLO”,JHEP12(2012) 061,doi:10.1007/JHEP12(2012)061,arXiv:1209.6215

  43. [43]

    Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions

    J. Alwall et al., “Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions”,Eur. Phys. J. C53(2008) 473, doi:10.1140/epjc/s10052-007-0490-5,arXiv:0706.2569

  44. [44]

    $W^{\pm}Z$ production at hadron colliders in NNLO QCD

    M. Grazzini, S. Kallweit, D. Rathlev, and M. Wiesemann, “W ±Z production at hadron colliders in NNLO QCD”,Phys. Lett. B761(2016) 179, doi:10.1016/j.physletb.2016.08.017,arXiv:1604.08576

  45. [45]

    Large electroweak corrections to vector-boson scattering at the Large Hadron Collider

    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, doi:10.1103/PhysRevLett.118.261801,arXiv:1611.02951

  46. [46]

    Complete NLO corrections to ${\rm W}^+{\rm W}^+$ scattering and its irreducible background at the LHC

    B. Biedermann, A. Denner, and M. Pellen, “Complete NLO corrections to W +W+ scattering and its irreducible background at the LHC”,JHEP10(2017) 124, doi:10.1007/JHEP10(2017)124,arXiv:1708.00268

  47. [47]

    QCD and electroweak corrections to WZ scattering at the LHC

    A. Denner et al., “QCD and electroweak corrections to WZ scattering at the LHC”,JHEP 06(2019) 067,doi:10.1007/JHEP06(2019)067,arXiv:1904.00882

  48. [48]

    Review of particle physics

    Particle Data Group Collaboration, “Review of particle physics”,Phys. Rev. D110(2024) 030001,doi:10.1103/PhysRevD.110.030001

  49. [49]

    Matching NLO QCD computations and parton shower simulations

    S. Frixione and B. R. Webber, “Matching NLO QCD computations and parton shower simulations”,JHEP06(2002) 029,doi:10.1088/1126-6708/2002/06/029, arXiv:hep-ph/0204244

  50. [50]

    A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms

    P . Nason, “A new method for combining NLO QCD with shower Monte Carlo algorithms”,JHEP11(2004) 040,doi:10.1088/1126-6708/2004/11/040, arXiv:hep-ph/0409146. References 21

  51. [51]

    Matching NLO QCD computations with Parton Shower simulations: the POWHEG method

    S. Frixione, P . Nason, and C. Oleari, “Matching NLO QCD computations with parton shower simulations: the POWHEG method”,JHEP11(2007) 070, doi:10.1088/1126-6708/2007/11/070,arXiv:0709.2092

  52. [52]

    NLO vector-boson production matched with shower in POWHEG

    S. Alioli, P . Nason, C. Oleari, and E. Re, “NLO vector-boson production matched with shower in POWHEG”,JHEP07(2008) 060, doi:10.1088/1126-6708/2008/07/060,arXiv:0805.4802

  53. [53]

    A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX

    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, doi:10.1007/JHEP06(2010)043,arXiv:1002.2581

  54. [54]

    Measurement of the associated production of a single top quark and a Z boson in pp collisions at $\sqrt{s} =$ 13 TeV

    CMS Collaboration, “Measurement of the associated production of a single top quark and a Z boson in pp collisions at √s= 13 TeV”,Phys. Lett. B779(2018) 358, doi:10.1016/j.physletb.2018.02.025,arXiv:1712.02825

  55. [55]

    A comprehensive guide to the physics and usage of PYTHIA 8.3

    C. Bierlich et al., “A comprehensive guide to the physics and usage of PYTHIA 8.3”, SciPost Phys. Codeb.2022(2022) 8,doi:10.21468/SciPostPhysCodeb.8, arXiv:2203.11601

  56. [56]

    Parton distributions from high-precision collider data

    NNPDF Collaboration, “Parton distributions from high-precision collider data”,Eur. Phys. J. C77(2017) 663,doi:10.1140/epjc/s10052-017-5199-5, arXiv:1706.00428

  57. [57]

    Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements

    CMS Collaboration, “Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements”,Eur. Phys. J. C80(2020) 4, doi:10.1140/epjc/s10052-019-7499-4,arXiv:1903.12179

  58. [58]

    Geant4 – a simulation toolkit

    GEANT4 Collaboration, “GEANT4 — a simulation toolkit”,Nucl. Instrum. Meth. A506 (2003) 250,doi:10.1016/S0168-9002(03)01368-8

  59. [59]

    Particle-flow reconstruction and global event description with the CMS detector

    CMS Collaboration, “Particle-flow reconstruction and global event description with the CMS detector”,JINST12(2017) P10003,doi:10.1088/1748-0221/12/10/P10003, arXiv:1706.04965

  60. [60]

    Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid

    CMS Collaboration, “Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid”, CMS Technical Proposal CERN-LHCC-2015-010, CMS-TDR-15-02, 2015

  61. [61]

    The anti-k_t jet clustering algorithm

    M. Cacciari, G. P . Salam, and G. Soyez, “The anti-kT jet clustering algorithm”,JHEP04 (2008) 063,doi:10.1088/1126-6708/2008/04/063,arXiv:0802.1189

  62. [62]

    FastJet user manual

    M. Cacciari, G. P . Salam, and G. Soyez, “FastJet user manual”,Eur. Phys. J. C72(2012) 1896,doi:10.1140/epjc/s10052-012-1896-2,arXiv:1111.6097

  63. [63]

    Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV

    CMS Collaboration, “Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV”,JINST12(2017) P02014, doi:10.1088/1748-0221/12/02/P02014,arXiv:1607.03663

  64. [64]

    Performance of missing transverse momentum reconstruction in proton-proton collisions at $\sqrt{s} =$ 13 TeV using the CMS detector

    CMS Collaboration, “Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector”,JINST14(2019) P07004,doi:10.1088/1748-0221/14/07/P07004,arXiv:1903.06078

  65. [65]

    Pileup mitigation at CMS in 13 TeV data

    CMS Collaboration, “Pileup mitigation at CMS in 13 TeV data”,JINST15(2020) P09018, doi:10.1088/1748-0221/15/09/P09018,arXiv:2003.00503. 22

  66. [66]

    Pileup Per Particle Identification

    D. Bertolini, P . Harris, M. Low, and N. Tran, “Pileup per particle identification”,JHEP10 (2014) 059,doi:10.1007/JHEP10(2014)059,arXiv:1407.6013

  67. [67]

    Particle Transformer for jet tagging

    H. Qu, C. Li, and S. Qian, “Particle Transformer for jet tagging”, inInternational Conference on Machine Learning, p. 18281, PMLR. 2022

  68. [68]

    Flavour tagging performance of the updated unified particle transformer algorithm with the cms experiment at √s=13 TeV

    CMS Collaboration, “Flavour tagging performance of the updated unified particle transformer algorithm with the cms experiment at √s=13 TeV”, CMS Detector Performance Summary CMS-DP-2025-081, 2025

  69. [69]

    Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at sqrt(s) = 8 TeV

    CMS Collaboration, “Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at √s=8 TeV”,JINST10(2015) P06005, doi:10.1088/1748-0221/10/06/P06005,arXiv:1502.02701

  70. [70]

    Measurements of properties of the Higgs boson decaying to a W boson pair in pp collisions at $\sqrt{s} =$ 13 TeV

    CMS Collaboration, “Measurements of properties of the Higgs boson decaying to a W boson pair in pp collisions at √s=13 TeV”,Phys. Lett. B791(2019) 96, doi:10.1016/j.physletb.2018.12.073,arXiv:1806.05246

  71. [71]

    Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying $\tau$ leptons at $\sqrt{s} =$ 13 TeV

    CMS Collaboration, “Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decayingτleptons at√s= 13 TeV”,JHEP08(2018) 066,doi:10.1007/JHEP08(2018)066, arXiv:1803.05485

  72. [72]

    Performance of CMS Muon Reconstruction in Cosmic-Ray Events

    CMS Collaboration, “Performance of CMS muon reconstruction in cosmic-ray events”, JINST5(2010) T03022,doi:10.1088/1748-0221/5/03/T03022, arXiv:0911.4994

  73. [73]

    Performance of the reconstruction and identification of high-momentum muons in proton-proton collisions at √s=13 TeV

    CMS Collaboration, “Performance of the reconstruction and identification of high-momentum muons in proton-proton collisions at √s=13 TeV”,JINST15(2020) P02027,doi:10.1088/1748-0221/15/02/P02027,arXiv:1912.03516

  74. [74]

    Probing color-singlet exchange in $Z+2$-jet events at the LHC

    D. L. Rainwater, R. Szalapski, and D. Zeppenfeld, “Probing color-singlet exchange inZ+ two jet events at the CERN LHC”,Phys. Rev. D54(1996) 6680, doi:10.1103/PhysRevD.54.6680,arXiv:hep-ph/9605444

  75. [75]

    TMVA - Toolkit for Multivariate Data Analysis

    H. Voss, A. H ¨ocker, J. Stelzer, and F. Tegenfeldt, “TMVA, the toolkit for multivariate data analysis with ROOT”, inXIth International Workshop on Advanced Computing and Analysis T echniques in Physics Research (ACAT), p. 40. 2007.arXiv:physics/0703039. doi:10.22323/1.050.0040

  76. [76]

    Electron and photon performance in CMS with the full 2017 data sample and additional 2016 highlights for the CALOR 2018 conference

    CMS Collaboration, “Electron and photon performance in CMS with the full 2017 data sample and additional 2016 highlights for the CALOR 2018 conference”, CMS Detector Performance Summary CMS-DP-2018-017, 2018

  77. [77]

    The CMS statistical analysis and combination tool: Combine

    CMS Collaboration, “The CMS statistical analysis and combination tool: COMBINE”, Comput. Softw. Big Sci.8(2024) 19,doi:10.1007/s41781-024-00121-4, arXiv:2404.06614

  78. [78]

    Asymptotic formulae for likelihood-based tests of new physics

    G. Cowan, K. Cranmer, E. Gross, and O. Vitells, “Asymptotic formulae for likelihood-based tests of new physics”,Eur. Phys. J. C71(2011) 1554, doi:10.1140/epjc/s10052-011-1554-0,arXiv:1007.1727. [Erratum: doi:10.1140/epjc/s10052-013-2501-z]

  79. [79]

    Luminosity measurement in proton-proton collisions at 13.6 TeV in 2022 at CMS

    CMS Collaboration, “Luminosity measurement in proton-proton collisions at 13.6 TeV in 2022 at CMS”, CMS Physics Analysis Summary CMS-PAS-LUM-22-001, 2024. References 23

  80. [80]

    Measurements of differential Z boson production cross sections in proton-proton collisions at √s= 13 TeV

    CMS Collaboration, “Measurements of differential Z boson production cross sections in proton-proton collisions at √s= 13 TeV”,JHEP12(2019) 061, doi:10.1007/JHEP12(2019)061,arXiv:1909.04133

Showing first 80 references.