pith. machine review for the scientific record. sign in

arxiv: 2605.14245 · v1 · submitted 2026-05-14 · ✦ hep-ex

Recognition: 2 theorem links

· Lean Theorem

Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the γγ final state in proton-proton collisions at sqrt{s} = 13 TeV

Authors on Pith no claims yet

Pith reviewed 2026-05-15 02:16 UTC · model grok-4.3

classification ✦ hep-ex
keywords bosonhiggscouplingsvectoranomalousbosonscandidateselectroweak
0
0 comments X

The pith

Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.

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

Physicists at CMS looked at Higgs bosons decaying into two photons using the entire 2016-2018 dataset. They sorted collision events into categories based on how the Higgs was produced: through gluon fusion, vector boson fusion, or together with a W or Z boson. Matrix element methods and machine learning discriminants helped separate signal from background. The analysis checked the CP properties of the Higgs-gluon coupling and the tensor structure of its interactions with electroweak bosons. No deviations from standard model predictions were observed in the fractional contributions of anomalous couplings to the production cross sections.

Core claim

The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.

Load-bearing premise

The matrix element techniques and multivariate discriminants correctly categorize events and separate signal from background without significant bias from unmodeled effects.

Figures

Figures reproduced from arXiv: 2605.14245 by CMS Collaboration.

Figure 1
Figure 1. Figure 1: LO SM Feynman diagrams for the (a) ggH, (b) VBF, and (c) VH production processes, [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Leading-order SM Feynman diagrams for the process in which a Higgs boson decay [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Topologies of the H production and decay, useful for the measurement of HVV cou [PITH_FULL_IMAGE:figures/full_fig_p012_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Distribution of the DVBF NNBSM (left) and DVBF 0− (right) discriminant for the SM VBF signal and for four anomalous coupling hypotheses, shown together with the main resonant back￾ground (SM ggH production), and the continuum diphoton background. The distributions are shown after the VBF preselection described in the text and are normalized to the unit area. The vertical dashed lines indicate the category … view at source ↗
Figure 5
Figure 5. Figure 5: Distributions of the DVBF NNBSM (left) and DVBF 0− (right) outputs for simulation (blue filled histograms, normalized to the data integral) and Drell-Yan data events (black markers). The corresponding ratio plots are shown in the bottom panels. The systematic uncertainty is esti￾mated by comparing NLO and LO Drell-Yan simulations, and is treated as a shape uncertainty [PITH_FULL_IMAGE:figures/full_fig_p01… view at source ↗
Figure 6
Figure 6. Figure 6: Output scores for the VH leptonic BDTs, D WHlep BSM (upper left), D ZHlep BSM (upper right), D VHMET BSM (lower) trained to separate the SM H signal from CP-odd (fa3 = 1) sample. The statis￾tical uncertainty in the data points is denoted as vertical bars and that on the background sim￾ulation by the gray/blue bars. The simulated signal and background distributions are normal￾ized to the luminosity of the d… view at source ↗
Figure 7
Figure 7. Figure 7: Signal and background distributions for the [PITH_FULL_IMAGE:figures/full_fig_p022_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: Definition of the Hgg analysis categories defined in bins of [PITH_FULL_IMAGE:figures/full_fig_p023_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: Examples of fits to the mγγ distribution for SM signal samples with mH = 125 GeV are shown for the luminosity-weighted average of the four data-taking periods, in two categories targeting VBF process, one dominated by SM-like (left) events and the other by BSM-like (right) events. Different Higgs boson production processes are summed according to their expected SM cross sections. The points represent simul… view at source ↗
Figure 10
Figure 10. Figure 10: Likelihood scan for the expected and observed constraints of the HVV anomalous [PITH_FULL_IMAGE:figures/full_fig_p028_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: Invariant mass distributions are presented separately for categories optimized for [PITH_FULL_IMAGE:figures/full_fig_p029_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: Distribution of events weighted by S/(S+B), using bins optimized for the VBF [PITH_FULL_IMAGE:figures/full_fig_p031_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: Data points (black) and signal-plus-background model fit for the sum of all the [PITH_FULL_IMAGE:figures/full_fig_p032_13.png] view at source ↗
Figure 14
Figure 14. Figure 14: Likelihood profile for the expected and observed constraints on [PITH_FULL_IMAGE:figures/full_fig_p032_14.png] view at source ↗
read the original abstract

Possible anomalous couplings of the Higgs boson to vector bosons and fermions are studied using Higgs boson candidates decaying to a pair of photons. The study is based on proton-proton collision data at $\sqrt{s}$ = 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. Events with Higgs boson candidates produced via gluon fusion, electroweak vector boson fusion and in association with a vector boson, are categorized using matrix element techniques and multivariate discriminants. The $CP$ properties of the Higgs boson couplings to gluons through loops of heavy particles, as well as the tensor structure of its interactions with two electroweak bosons, are investigated. The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.

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

0 major / 2 minor

Summary. The manuscript reports constraints on anomalous Higgs boson couplings to vector bosons and fermions using the diphoton decay channel in 138 fb^{-1} of 13 TeV proton-proton collision data collected by CMS. Events are categorized into gluon-fusion, vector-boson-fusion, and associated-production modes via matrix-element techniques and multivariate discriminants; the CP properties of the gluon couplings and the tensor structure of the electroweak couplings are examined. Results are presented as fractional contributions of anomalous couplings to each production cross section and found consistent with Standard Model expectations.

Significance. If the central results hold, the work supplies competitive, data-driven limits on dimension-6 operator contributions to Higgs production, exploiting the clean diphoton final state and a large dataset. The combination of matrix-element discriminants, BDT categorization, and a binned likelihood fit to the diphoton mass plus discriminant outputs constitutes a standard yet robust EFT-style analysis whose consistency checks (closure tests, control-region validation) support the reported SM agreement.

minor comments (2)
  1. [Abstract] The abstract states consistency with SM expectations but omits any quantitative indication of the fit uncertainties or the dominant systematic sources; adding a single sentence summarizing the leading uncertainties would improve readability without altering the technical content.
  2. [Signal modeling] Section describing the signal reweighting procedure should explicitly state the range of anomalous coupling values used to generate the templates and confirm that the reweighting preserves the normalization of the SM component.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the careful reading and positive assessment of the manuscript. The analysis provides updated constraints on anomalous Higgs boson couplings to vector bosons and fermions in the diphoton channel using the full Run 2 dataset of 138 fb^{-1}. The results remain consistent with Standard Model expectations across gluon-fusion, vector-boson-fusion, and associated-production modes. No major comments were raised in the report.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The analysis assumes standard model background shapes and signal templates from simulation, with no new free parameters or invented entities introduced beyond the coupling fractions being constrained.

axioms (1)
  • domain assumption Standard model predictions for Higgs production cross sections and decay branching ratios are accurate enough for background subtraction and signal modeling.
    Invoked implicitly in event categorization and interpretation of fractional contributions.

pith-pipeline@v0.9.0 · 5456 in / 1139 out tokens · 43004 ms · 2026-05-15T02:16:49.728489+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

93 extracted references · 93 canonical work pages · 51 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]

    Partial-symmetries of weak interactions

    S. L. Glashow, “Partial-symmetries of weak interactions”,Nucl. Phys.22(1961) 579, doi:10.1016/0029-5582(61)90469-2

  5. [5]

    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

  6. [6]

    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

  7. [7]

    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

  8. [8]

    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

  9. [9]

    A model of leptons

    S. Weinberg, “A model of leptons”,Phys. Rev. Lett.19(1967) 1264, doi:10.1103/PhysRevLett.19.1264

  10. [10]

    Weak and electromagnetic interactions

    A. Salam, “Weak and electromagnetic interactions”,Conf. Proc. C680519(1968) 367, doi:10.1142/9789812795915_0034

  11. [11]

    Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV

    CMS Collaboration, “Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV”,Phys. Rev. D92(2015) 012004, doi:10.1103/PhysRevD.92.012004,arXiv:1411.3441

  12. [12]

    Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector

    ATLAS Collaboration, “Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector”,Eur. Phys. J. C75(2015) 476, doi:10.1140/epjc/s10052-015-3685-1,arXiv:1506.05669. 34

  13. [13]

    Study of the mass and spin-parity of the Higgs boson candidate via its decays to Z boson pairs

    CMS Collaboration, “Study of the mass and spin-parity of the Higgs boson candidate via its decays to Z boson pairs”,Phys. Rev. Lett.110(2013) 081803, doi:10.1103/PhysRevLett.110.081803,arXiv:1212.6639

  14. [14]

    Measurement of the properties of a Higgs boson in the four-lepton final state

    CMS Collaboration, “Measurement of the properties of a Higgs boson in the four-lepton final state”,Phys. Rev. D89(2014) 092007,doi:10.1103/PhysRevD.89.092007, arXiv:1312.5353

  15. [15]

    Limits on the Higgs boson lifetime and width from its decay to four charged leptons

    CMS Collaboration, “Limits on the Higgs boson lifetime and width from its decay to four charged leptons”,Phys. Rev. D92(2015) 072010, doi:10.1103/PhysRevD.92.072010,arXiv:1507.06656

  16. [16]

    Combined search for anomalous pseudoscalar HVV couplings in VH production and H to VV decay

    CMS Collaboration, “Combined search for anomalous pseudoscalar HVV couplings in VH production and H→VV decay”,Phys. Lett. B759(2016) 672, doi:10.1016/j.physletb.2016.06.004,arXiv:1602.04305

  17. [17]

    Constraints on anomalous Higgs boson couplings using production and decay information in the four-lepton final state

    CMS Collaboration, “Constraints on anomalous Higgs boson couplings using production and decay information in the four-lepton final state”,Phys. Lett. B775(2017) 1, doi:10.1016/j.physletb.2017.10.021,arXiv:1707.00541

  18. [18]

    Measurements of the Higgs boson width and anomalous HVV couplings from on-shell and off-shell production in the four-lepton final state

    CMS Collaboration, “Measurements of the Higgs boson width and anomalous HVV couplings from on-shell and off-shell production in the four-lepton final state”,Phys. Rev. D99(2019) 112003,doi:10.1103/PhysRevD.99.112003,arXiv:1901.00174

  19. [19]

    Constraints on anomalous HVV couplings from the production of Higgs bosons decaying toτlepton pairs

    CMS Collaboration, “Constraints on anomalous HVV couplings from the production of Higgs bosons decaying toτlepton pairs”,Phys. Rev. D100(2019) 112002, doi:10.1103/PhysRevD.100.112002,arXiv:1903.06973

  20. [20]

    Measurements of t ¯tH production and theCPstructure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel

    CMS Collaboration, “Measurements of t ¯tH production and theCPstructure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel”,Phys. Rev. Lett.125(2020) 061801, doi:10.1103/PhysRevLett.125.061801,arXiv:2003.10866

  21. [21]

    Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state

    CMS Collaboration, “Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state”,Phys. Rev. D 104(2021) 052004,doi:10.1103/PhysRevD.104.052004,arXiv:2104.12152

  22. [22]

    Analysis of theCPstructure of the Yukawa coupling between the Higgs boson andτleptons in proton-proton collisions at √s=13 TeV

    CMS Collaboration, “Analysis of theCPstructure of the Yukawa coupling between the Higgs boson andτleptons in proton-proton collisions at √s=13 TeV”,JHEP06(2022) 012,doi:10.1007/jhep06(2022)012,arXiv:2110.04836

  23. [23]

    Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production

    CMS Collaboration, “Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production”,Nature Phys.18(2022) 1329, doi:10.1038/s41567-022-01682-0,arXiv:2202.06923

  24. [24]

    Evidence for the spin-0 nature of the Higgs boson using ATLAS data

    ATLAS Collaboration, “Evidence for the spin-0 nature of the Higgs boson using ATLAS data”,Phys. Lett. B726(2013) 120,doi:10.1016/j.physletb.2013.08.026, arXiv:1307.1432

  25. [25]

    Test of CP Invariance in vector-boson fusion production of the Higgs boson using the Optimal Observable method in the ditau decay channel with the ATLAS detector

    ATLAS Collaboration, “Test of CP invariance in vector-boson fusion production of the Higgs boson using the optimal observable method in the ditau decay channel with the ATLAS detector”,Eur. Phys. J. C76(2016) 658, doi:10.1140/epjc/s10052-016-4499-5,arXiv:1602.04516. References 35

  26. [26]

    Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

    ATLAS Collaboration, “Measurement of inclusive and differential cross sections in the H→ZZ ∗ →4ℓdecay channel in pp collisions at √s=13 TeV with the ATLAS detector”, JHEP10(2017) 132,doi:10.1007/JHEP10(2017)132,arXiv:1708.02810

  27. [27]

    Measurement of the Higgs boson coupling properties in the $H\rightarrow ZZ^{*} \rightarrow 4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector

    ATLAS Collaboration, “Measurement of the Higgs boson coupling properties in the H→ZZ ∗ →4ℓdecay channel at √s=13 TeV with the ATLAS detector”,JHEP03 (2018) 095,doi:10.1007/JHEP03(2018)095,arXiv:1712.02304

  28. [28]

    Measurements of Higgs boson properties in the diphoton decay channel with 36 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector

    ATLAS Collaboration, “Measurements of Higgs boson properties in the diphoton decay channel with 36 fb−1 of pp collision data at √s=13 TeV with the ATLAS detector”,Phys. Rev. D98(2018) 052005,doi:10.1103/PhysRevD.98.052005,arXiv:1802.04146

  29. [29]

    Test of CP invariance in vector-boson fusion production of the Higgs boson in the H→ττchannel in proton-proton collisions at √s=13 TeV with the ATLAS detector

    ATLAS Collaboration, “Test of CP invariance in vector-boson fusion production of the Higgs boson in the H→ττchannel in proton-proton collisions at √s=13 TeV with the ATLAS detector”,Phys. Lett. B805(2020) 135426, doi:10.1016/j.physletb.2020.135426,arXiv:2002.05315

  30. [30]

    CPproperties of Higgs boson interactions with top quarks in the ttH and tH processes using H→γγwith the ATLAS detector

    ATLAS Collaboration, “CPproperties of Higgs boson interactions with top quarks in the ttH and tH processes using H→γγwith the ATLAS detector”,Phys. Rev. Lett.125 (2020) 061802,doi:10.1103/PhysRevLett.125.061802,arXiv:2004.04545

  31. [31]

    Constraints on Higgs boson properties using WW ∗(→eνµν)jj production in 36.1 fb−1 of √s=13 TeV pp collisions with the ATLAS detector

    ATLAS Collaboration, “Constraints on Higgs boson properties using WW ∗(→eνµν)jj production in 36.1 fb−1 of √s=13 TeV pp collisions with the ATLAS detector”, 2022. arXiv:2109.13808. Published inEur. Phys. J. C

  32. [32]

    Determining the cp nature of a neutral higgs boson at the cern large hadron collider

    J. F. Gunion and X.-G. He, “Determining the cp nature of a neutral higgs boson at the cern large hadron collider”,Phys. Rev. Lett.76(Jun, 1996) 4468, doi:10.1103/PhysRevLett.76.4468

  33. [33]

    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

  34. [34]

    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, arXiv:2309.05466

  35. [35]

    Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton-proton collisions at√s=13 TeV

    CMS Collaboration, “Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton-proton collisions at√s=13 TeV”,Eur. Phys. J. C84(2024) 779, doi:10.1140/epjc/s10052-024-12925-0,arXiv:2403.00657

  36. [36]

    Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using theττfinal state

    CMS Collaboration, “Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using theττfinal state”,Phys. Rev. D 108(2023) 032013,doi:10.1103/PhysRevD.108.032013,arXiv:2205.05120

  37. [37]

    HEPData record for this analysis, 2026.doi:10.17182/hepdata.169546

  38. [38]

    Determining the Structure of Higgs Couplings at the LHC

    T. Plehn, D. L. Rainwater, and D. Zeppenfeld, “Determining the structure of Higgs couplings at the LHC”,Phys. Rev. Lett.88(2002) 051801, doi:10.1103/PhysRevLett.88.051801,arXiv:hep-ph/0105325

  39. [39]

    Anomalous Higgs boson couplings in vector boson fusion at the CERN LHC

    V . Hankele, G. Klamke, D. Zeppenfeld, and T. Figy, “Anomalous Higgs boson couplings in vector boson fusion at the CERN LHC”,Phys. Rev. D74(2006) 095001, doi:10.1103/PhysRevD.74.095001,arXiv:hep-ph/0609075. 36

  40. [40]

    Proceedings of the Workshop on CP studies and non-standard Higgs physics

    S. Kraml et al., “Proceedings of the Workshop on CP studies and non-standard Higgs physics”, inProc. Workshop on CP studies and non-standard Higgs physics. 2006. arXiv:hep-ph/0608079.doi:10.5170/CERN-2006-009

  41. [41]

    Jet angular correlation in vector-boson fusion processes at hadron colliders

    K. Hagiwara, Q. Li, and K. Mawatari, “Jet angular correlation in vector-boson fusion processes at hadron colliders”,JHEP07(2009) 101, doi:10.1088/1126-6708/2009/07/101,arXiv:0905.4314

  42. [42]

    Spin determination of single-produced resonances at hadron colliders

    Y. Gao et al., “Spin determination of single-produced resonances at hadron colliders”, Phys. Rev. D81(2010) 075022,doi:10.1103/PhysRevD.81.075022, arXiv:1001.3396

  43. [43]

    Higgs look-alikes at the LHC

    A. De Rujula et al., “Higgs look-alikes at the LHC”,Phys. Rev. D82(2010) 013003, doi:10.1103/PhysRevD.82.013003,arXiv:1001.5300

  44. [44]

    On the spin and parity of a single-produced resonance at the LHC

    S. Bolognesi et al., “Spin and parity of a single-produced resonance at the LHC”,Phys. Rev. D86(2012) 095031,doi:10.1103/PhysRevD.86.095031,arXiv:1208.4018

  45. [45]

    A Fast Track towards the `Higgs' Spin and Parity

    J. Ellis, D. S. Hwang, V . Sanz, and T. You, “A fast track towards the ’Higgs’ spin and parity”,JHEP11(2012) 134,doi:10.1007/JHEP11(2012)134,arXiv:1208.6002

  46. [46]

    A framework for Higgs characterisation

    P . Artoisenet et al., “A framework for Higgs characterisation”,JHEP11(2013) 043, doi:10.1007/JHEP11(2013)043,arXiv:1306.6464

  47. [47]

    Constraining anomalous HVV interactions at proton and lepton colliders

    I. Anderson et al., “Constraining anomalous HVV interactions at proton and lepton colliders”,Phys. Rev. D89(2014) 035007,doi:10.1103/PhysRevD.89.035007, arXiv:1309.4819

  48. [48]

    Constraining CP-violating Higgs Sectors at the LHC using gluon fusion

    M. J. Dolan, P . Harris, M. Jankowiak, and M. Spannowsky, “ConstrainingCP-violating Higgs sectors at the LHC using gluon fusion”,Phys. Rev. D90(2014) 073008, doi:10.1103/PhysRevD.90.073008,arXiv:1406.3322

  49. [49]

    Pseudo-observables in electroweak Higgs production

    A. Greljo, G. Isidori, J. M. Lindert, and D. Marzocca, “Pseudo-observables in electroweak Higgs production”,Eur. Phys. J. C76(2016) 158, doi:10.1140/epjc/s10052-016-4000-5,arXiv:1512.06135

  50. [50]

    Constraining anomalous Higgs boson couplings to the heavy flavor fermions using matrix element techniques

    A. V . Gritsan, R. R¨ontsch, M. Schulze, and M. Xiao, “Constraining anomalous Higgs boson couplings to the heavy flavor fermions using matrix element techniques”,Phys. Rev. D94(2016) 055023,doi:10.1103/PhysRevD.94.055023,arXiv:1606.03107

  51. [51]

    Constraining anomalous Higgs boson couplings to virtual photons

    J. Davis et al., “Constraining anomalous Higgs boson couplings to virtual photons”, Phys. Rev. D105(2022) 096027,doi:10.1103/PhysRevD.105.096027, arXiv:2109.13363

  52. [52]

    New features in the JHU generator framework: constraining Higgs boson properties from on-shell and off-shell production

    A. V . Gritsan et al., “New features in the JHU generator framework: constraining Higgs boson properties from on-shell and off-shell production”,Phys. Rev. D102(2020) 056022, doi:10.1103/PhysRevD.102.056022,arXiv:2002.09888

  53. [53]

    Finite quark-mass effects in the NNLOPS POWHEG+MiNLO Higgs generator

    K. Hamilton, P . Nason, and G. Zanderighi, “Finite quark-mass effects in the NNLOPS POWHEG+MiNLO Higgs generator”,JHEP05(2015) 140, doi:10.1007/JHEP05(2015)140,arXiv:1501.04637

  54. [54]

    Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV

    CMS Collaboration, “Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV”,JHEP07(2021) 027, doi:10.1007/JHEP07(2021)027,arXiv:2103.06956. References 37

  55. [55]

    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

  56. [56]

    The CMS trigger system

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

  57. [57]

    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

  58. [58]

    Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS

    CMS Collaboration, “Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS”,Eur. Phys. J. C81(2021) 800, doi:10.1140/epjc/s10052-021-09538-2,arXiv:2104.01927

  59. [59]

    CMS luminosity measurement for the 2017 data-taking period at√s=13 TeV

    CMS Collaboration, “CMS luminosity measurement for the 2017 data-taking period at√s=13 TeV”, CMS Physics Analysis Summary CMS-PAS-LUM-17-004, 2018

  60. [60]

    CMS luminosity measurement for the 2018 data-taking period at√s=13 TeV

    CMS Collaboration, “CMS luminosity measurement for the 2018 data-taking period at√s=13 TeV”, CMS Physics Analysis Summary CMS-PAS-LUM-18-002, 2019

  61. [61]

    Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at √s=7 TeV

    CMS Collaboration, “Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at √s=7 TeV”,JHEP10(2011) 132,doi:10.1007/JHEP10(2011)132

  62. [62]

    An Introduction to PYTHIA 8.2

    T. Sj ¨ostrand et al., “An introduction toPYTHIA8.2”,Comput. Phys. Commun.191(2015) 159,doi:10.1016/j.cpc.2015.01.024,arXiv:1410.3012

  63. [63]

    Event generator tunes obtained from underlying event and multiparton scattering measurements

    CMS Collaboration, “Event generator tunes obtained from underlying event and multiparton scattering measurements”,Eur. Phys. J. C76(2016) 155, doi:10.1140/epjc/s10052-016-3988-x,arXiv:1512.00815

  64. [64]

    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

  65. [65]

    Parton distributions for the LHC Run II

    NNPDF Collaboration, “Parton distributions for the LHC Run II”,JHEP04(2015) 040, doi:10.1007/JHEP04(2015)040,arXiv:1410.8849

  66. [66]

    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

  67. [67]

    Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector

    LHC Higgs Cross Section Working Group, “Handbook of LHC Higgs Cross Sections: 4. Deciphering the nature of the Higgs sector”,CERN Y ellow Rep. Monogr.2(2017) doi:10.23731/CYRM-2017-002,arXiv:1610.07922

  68. [68]

    GEANT4 — a simulation toolkit

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

  69. [69]

    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

  70. [70]

    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. 38

  71. [71]

    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

  72. [72]

    NLO Higgs boson production via gluon fusion matched with shower in POWHEG

    S. Alioli, P . Nason, C. Oleari, and E. Re, “NLO Higgs boson production via gluon fusion matched with shower in POWHEG”,JHEP04(2009) 002, doi:10.1088/1126-6708/2009/04/002,arXiv:0812.0578

  73. [73]

    NLO Higgs boson production via vector-boson fusion matched with shower in POWHEG

    P . Nason and C. Oleari, “NLO Higgs boson production via vector-boson fusion matched with shower inPOWHEG”,JHEP02(2010) 037,doi:10.1007/JHEP02(2010)037, arXiv:0911.5299

  74. [74]

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

  75. [75]

    Higgs boson production in association with top quarks in the POWHEG BOX

    H. B. Hartanto, B. J ¨ager, L. Reina, and D. Wackeroth, “Higgs boson production in association with top quarks in thePOWHEGBOX”,Phys. Rev. D91(2015) 094003, doi:10.1103/PhysRevD.91.094003,arXiv:1501.04498

  76. [76]

    An interface between thePOWHEG BOXand MADGRAPH5 aMC@NLO

    P . Nason, C. Oleari, M. Rocco, and M. Zaro, “An interface between thePOWHEG BOXand MADGRAPH5 aMC@NLO”,Eur. Phys. J. C80(2020) 10, doi:10.1140/epjc/s10052-020-08559-7,arXiv:2008.06364

  77. [77]

    Event generation with SHERPA 1.1

    T. Gleisberg et al., “Event generation with SHERPA 1.1”,JHEP02(2009) 007, doi:10.1088/1126-6708/2009/02/007,arXiv:0811.4622

  78. [78]

    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

  79. [79]

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

    A. M. Sirunyan et al., “Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC”,Journal of Instrumentation16(2021) doi:10.1088/1748-0221/16/05/p05014

  80. [80]

    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

Showing first 80 references.