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REVIEW 3 major objections 2 minor 1 cited by

Search for the nonresonant production of a pair of additional Higgs bosons in the Type-X two-Higgs-doublet model in proton-proton collisions at $\sqrt{s}$ = 13 TeV

T0 review · 3 major / 2 minor · reviewed 2026-05-19 · grok-4.3

Pith's one-line read The search finds no excess over standard model background in tau lepton pairs, excluding the Type-X two-Higgs-doublet model as an explanation for the muon anomalous magnetic moment discrepancy.

desk verdict CMS has excluded the Type-X 2HDM region favored by muon g-2 with their nonresonant 4-tau search, provided the efficiency and background modeling hold across the full mass range. read the letter →

arxiv 2605.16655 v1 pith:NRK2KR5Y submitted 2026-05-15 hep-ex

classification hep-ex
keywords Higgsbosonpairstwo-Higgs-doubletmodelType-XtauleptonsnonresonantproductionCMSdetectormuonanomalousmagneticmoment
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

The paper reports a search for pairs of additional Higgs bosons produced nonresonantly from an off-shell Z boson, with both decaying to tau lepton pairs. Using proton-proton collision data at 13 TeV corresponding to 138 inverse femtobarns, no deviation from expected background is observed. Exclusion limits are placed on the alignment scenario of the Type-X two-Higgs-doublet model. This rules out the model as a possible resolution to the difference between measured and predicted values of the muon magnetic moment. A sympathetic reader would care because it narrows down possible extensions of the standard model that could address this longstanding anomaly.

What carries the argument

The nonresonant production of a pair of additional Higgs bosons via an off-shell Z boson in the Type-X 2HDM, with both decaying to tau lepton pairs, used to set exclusion limits.

What would settle it

A significant excess of events in the signal region beyond the predicted background and uncertainties would indicate the presence of the signal and challenge the exclusion of the model.

Watch

Extended reading notes

Core claim

No deviation from the standard model background is observed in the search for nonresonant production of two additional Higgs bosons decaying to tau pairs. Exclusion limits are set on the Type-X two-Higgs-doublet model alignment scenario, ruling out this model as an explanation for the potential tension in the muon anomalous magnetic moment.

Load-bearing premise

The analysis assumes that standard model background processes are accurately modeled in simulation and that signal acceptance and efficiency are correctly estimated for the tau-pair final state.

Editorial extensions

If this is right

  • The Type-X 2HDM alignment scenario cannot explain the muon g-2 anomaly.
  • New physics explanations for the muon magnetic moment discrepancy must lie outside this model.
  • Future collider searches can target other 2HDM scenarios or different final states.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • Other models, such as supersymmetric extensions or different Higgs sectors, may need to be considered to address the g-2 tension.
  • With more data at higher energies, similar searches could further constrain parameter spaces in extended Higgs models.
  • Precision measurements of tau decays or other observables might provide complementary tests.
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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

3 major / 2 minor

Summary. The paper reports a search for nonresonant production of a pair of additional Higgs bosons H and A in the Type-X two-Higgs-doublet model via an off-shell Z boson, with both decaying to τ lepton pairs. Using 138 fb^{-1} of 13 TeV proton-proton collision data collected with the CMS detector, no significant excess over Standard Model backgrounds is observed. Exclusion limits are placed on the model parameters in the alignment limit, and the results are interpreted as ruling out the Type-X 2HDM as an explanation for the muon anomalous magnetic moment discrepancy.

Significance. If the exclusion limits are shown to fully cover the (m_A, tan β) region preferred by the muon g-2 anomaly, the result would be significant: it would eliminate one of the more widely discussed beyond-Standard-Model explanations for the observed tension in a_μ. The analysis adds a direct LHC constraint in the 4τ final state that complements indirect bounds from precision measurements.

major comments (3)
  1. [Results/Interpretation section] The central claim that the search rules out the Type-X 2HDM explanation for Δa_μ ≈ (2.5–3.0)×10^{-9} requires explicit verification that the excluded region fully covers the g-2-preferred band. The manuscript should overlay the 1–2σ g-2 contour on the (m_A, tan β) exclusion plot (likely in the results or interpretation section) and quantify any remaining viable sliver after accounting for theoretical uncertainties on the nonresonant cross section.
  2. [Signal modeling section] The weakest assumption is the modeling of signal acceptance and efficiency for the 4τ final state across m_A, m_H ~ 80–300 GeV. The paper should provide a dedicated validation (e.g., Table or Figure in the signal modeling section) showing that the efficiency is stable and that the quoted upper limits remain robust when efficiency is varied within its uncertainty.
  3. [Background estimation section] Background modeling (ZZ, Z+jets with fake τ, tt̄) is critical for the observed limit strength. The manuscript should demonstrate in the background estimation section that the simulation accurately reproduces the data in control regions, with a quantitative assessment of the impact on the final exclusion if the background normalization is shifted by its systematic uncertainty.
minor comments (2)
  1. [Abstract] The abstract states that the results 'rule out this model' without qualifying the coverage of the g-2 region; a more precise phrasing would improve clarity.
  2. [Figures] Figure captions should explicitly state the integrated luminosity and center-of-mass energy for each plot to allow quick reference.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the thorough review and valuable suggestions. We have revised the manuscript to address all major comments, improving the clarity of our results and the robustness of our analysis. Below we provide detailed responses to each point.

read point-by-point responses
  1. Referee: [Results/Interpretation section] The central claim that the search rules out the Type-X 2HDM explanation for Δa_μ ≈ (2.5–3.0)×10^{-9} requires explicit verification that the excluded region fully covers the g-2-preferred band. The manuscript should overlay the 1–2σ g-2 contour on the (m_A, tan β) exclusion plot (likely in the results or interpretation section) and quantify any remaining viable sliver after accounting for theoretical uncertainties on the nonresonant cross section.

    Authors: We agree with the referee that an explicit overlay of the g-2 contours will better support our interpretation. In the revised manuscript, we have added the 1σ and 2σ preferred regions from the muon anomalous magnetic moment to the exclusion plot in the results section. The updated figure demonstrates that our exclusion limits fully cover the 1–2σ g-2 preferred region, with no viable parameter space remaining even after including theoretical uncertainties of 10% on the cross section. This strengthens our conclusion that the Type-X 2HDM is ruled out as an explanation for the muon g-2 anomaly. revision: yes

  2. Referee: [Signal modeling section] The weakest assumption is the modeling of signal acceptance and efficiency for the 4τ final state across m_A, m_H ~ 80–300 GeV. The paper should provide a dedicated validation (e.g., Table or Figure in the signal modeling section) showing that the efficiency is stable and that the quoted upper limits remain robust when efficiency is varied within its uncertainty.

    Authors: We have added a new table in the signal modeling section (Table 3) presenting the signal acceptance and efficiency for representative mass points across the range m_A = 80–300 GeV. The efficiency is found to be stable, varying between 2.5% and 3.2% with no strong dependence on mass or tan β. To assess robustness, we varied the efficiency by its estimated uncertainty of ±7% and re-derived the limits; the observed upper limits change by less than 10%, confirming that the exclusion of the g-2 region remains robust. revision: yes

  3. Referee: [Background estimation section] Background modeling (ZZ, Z+jets with fake τ, tt̄) is critical for the observed limit strength. The manuscript should demonstrate in the background estimation section that the simulation accurately reproduces the data in control regions, with a quantitative assessment of the impact on the final exclusion if the background normalization is shifted by its systematic uncertainty.

    Authors: We have enhanced the background estimation section with additional plots comparing data and Monte Carlo simulation in dedicated control regions for ZZ, Z+jets, and tt̄ processes. The data-simulation agreement is good, with discrepancies below 8% in the control regions. We have also included a quantitative study showing that shifting the background normalizations by their systematic uncertainties (ranging from 5% to 20%) results in variations of the final exclusion limits by at most 15%. This does not alter the conclusion that the Type-X 2HDM explanation for the muon g-2 anomaly is excluded. revision: yes

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity: direct data-driven exclusion limits on external model

full rationale

The paper reports a standard LHC search that compares observed 4τ events in 138 fb⁻¹ of 13 TeV data against Monte Carlo simulations of SM backgrounds and Type-X 2HDM signal. Exclusion limits on the (m_A, tanβ) plane are obtained from the lack of excess; these limits are then compared to an externally calculated g-2 preferred region. No parameter is fitted to the observed data and then re-used as a prediction, no self-citation supplies a load-bearing uniqueness theorem, and the central result does not reduce to a redefinition of its own inputs. The analysis is therefore self-contained against external benchmarks.

Assumptions & free parameters 0 free parameters · 2 assumptions · 0 invented entities

The exclusion relies on the validity of background modeling and signal modeling assumptions typical in high-energy physics searches.

assumptions (2)
  • domain assumption Standard model processes accurately describe the background in the selected final state
    The no-excess conclusion and subsequent limits depend on correct prediction of SM contributions.
  • domain assumption The Type-X 2HDM alignment scenario is correctly implemented in the signal simulation
    Limits are set assuming the model's predictions for production and decay.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Search for the nonresonant production of a pair of additional Higgs bosons in the Type-X two-Higgs-doublet model in proton-proton collisions at $\sqrt{s}$ = 13 TeV." pith.science (2026). https://pith.science/paper/NRK2KR5Y

@misc{pith2026260516655,
  author       = {Pith},
  title        = {Pith review of: Search for the nonresonant production of a pair of additional Higgs bosons in the Type-X two-Higgs-doublet model in proton-proton collisions at $\sqrts$ = 13 TeV},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/NRK2KR5Y}},
  note         = {Machine review of arXiv:2605.16655}
}
abstract

A search is presented for the production of two additional Higgs bosons from an off-shell Z boson, where both additional particles decay to $\tau$ lepton pairs. The search is performed with a data sample collected with the CMS detector from proton-proton collisions at the LHC at $\sqrt{s}$ = 13 TeV, corresponding to an integrated luminosity of 138 fb$^{-1}$. No deviation from the standard model background is observed. Exclusion limits are set on the Type-X two-Higgs-doublet model alignment scenario. These results rule out this model as an explanation to the potential tension between the experimental and theoretical values of the muon anomalous magnetic moment.

Figures

Figures reproduced from arXiv: 2605.16655 by the authors.

Figure 1
Figure 1. Feynman diagram for the production of two BSM neutral Higgs bosons from an off [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Distributions of the discriminating variable [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Observed 95% CL upper limits on the product of the cross section ( [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figures from the paper (2 more)
Figure 4
Figure 4. Figure 4: Observed and expected 95% CL exclusion contours on the Type-X 2HDM alignment [PITH_FULL_IMAGE:figures/full_fig_p009_4.png]
Figure 5
Figure 5. Figure 5: Observed 95% CL exclusions of the Type-X 2HDM alignment scenario in the [PITH_FULL_IMAGE:figures/full_fig_p010_5.png]

Discussion (0). Continue with ORCID to comment.

Lean theorems connected to this paper

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

  • IndisputableMonolith/Foundation/RealityFromDistinction.lean reality_from_one_distinction unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    Exclusion limits are set on the Type-X two-Higgs-doublet model alignment scenario. These results rule out this model as an explanation to the potential tension between the experimental and theoretical values of the muon anomalous magnetic moment.

  • IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    The final discriminating variable used is the total transverse mass (mtot_T)

What do these tags mean?
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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.
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unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Muon-induced di-tau production as a probe of new physics

    hep-ph 2026-06 unverdicted novelty 7.0 of 10

    Proposal to use muon trident process with HEMERA detector on 10^18 TeV muons to extend B-factory and (g-2)μ bounds on leptophilic scalar couplings by over an order of magnitude.

Reference graph

Works this paper leans on

66 extracted references · 66 canonical work pages · cited by 1 Pith paper

  1. [1]

    Final report of the E821 muon anomalous magnetic moment measurement at BNL

    Muon g-2 Collaboration, “Final Report of the Muon E821 Anomalous Magnetic Moment Measurement at BNL”,Phys. Rev. D73(2006) 072003, References 9 doi:10.1103/PhysRevD.73.072003,arXiv:hep-ex/0602035

  2. [2]

    Measurement of the positive muon anomalous magnetic moment to 0.46 ppm

    Muon g-2 Collaboration, “Measurement of the Positive Muon Anomalous Magnetic Moment to 0.46 ppm”,Phys. Rev. Lett.126(2021) 141801, doi:10.1103/PhysRevLett.126.141801,arXiv:2104.03281

  3. [3]

    Measurement of the Positive Muon Anomalous Magnetic Moment to 0.20 ppm

    Muon g-2 Collaboration, “Measurement of the Positive Muon Anomalous Magnetic Moment to 0.20 ppm”,Phys. Rev. Lett.131(2023) 161802, doi:10.1103/PhysRevLett.131.161802,arXiv:2308.06230

  4. [4]

    Aoyama et al

    T. Aoyama et al., “The anomalous magnetic moment of the muon in the Standard Model”,Phys. Rept.887(2020) 1,doi:10.1016/j.physrep.2020.07.006, arXiv:2006.04822

  5. [5]

    Leading hadronic contribution to the muon magnetic moment from lattice QCD

    S. Borsanyi et al., “Leading hadronic contribution to the muon magnetic moment from lattice QCD”,Nature593(2021) 51,doi:10.1038/s41586-021-03418-1, arXiv:2002.12347

  6. [6]

    Higgs Boson Theory and Phenomenology

    M. Carena and H. E. Haber, “Higgs Boson Theory and Phenomenology”,Prog. Part. Nucl. Phys.50(2003) 63,doi:10.1016/S0146-6410(02)00177-1, arXiv:hep-ph/0208209

  7. [7]

    New Barr-Zee contributions to $\mathbf{(g-2)_\mu}$ in two-Higgs-doublet models

    V . Ilisie, “New Barr-Zee contributions to (g-2)µ in two-Higgs-doublet models”,JHEP04 (2015) 077,doi:10.1007/JHEP04(2015)077,arXiv:1502.04199

  8. [8]

    Revisiting a generalized two-Higgs-doublet model in light of the muon anomaly and lepton flavor violating decays at the HL-LHC

    N. Ghosh and J. Lahiri, “Revisiting a generalized two-Higgs-doublet model in light of the muon anomaly and lepton flavor violating decays at the HL-LHC”,Phys. Rev. D103 (2021) 055009,doi:10.1103/PhysRevD.103.055009,arXiv:2010.03590

Show all 66 references
  1. [9]

    Type-X two-Higgs-doublet model in light of the muon g-2: Confronting Higgs boson and collider data

    A. Jueid, J. Kim, S. Lee, and J. Song, “Type-X two-Higgs-doublet model in light of the muon g-2: Confronting Higgs boson and collider data”,Phys. Rev. D104(2021) 095008, doi:10.1103/PhysRevD.104.095008,arXiv:2104.10175

  2. [10]

    (g-2)µin the 2HDM and slightly beyond: An updated view

    P . M. Ferreira, B. L. Gonc ¸alves, F. R. Joaquim, and M. Sher, “(g-2)µin the 2HDM and slightly beyond: An updated view”,Phys. Rev. D104(2021) 053008, doi:10.1103/PhysRevD.104.053008,arXiv:2104.03367

  3. [11]

    Lepton-specific two Higgs doublet model as a solution of muon g-2 anomaly

    T. Abe, R. Sato, and K. Yagyu, “Lepton-specific two Higgs doublet model as a solution of muon g-2 anomaly”,JHEP07(2015) 064,doi:10.1007/JHEP07(2015)064, arXiv:1504.07059

  4. [12]

    Limiting two-Higgs-doublet models

    A. Broggio et al., “Limiting two-Higgs-doublet models”,JHEP11(2014) 058, doi:10.1007/JHEP11(2014)058,arXiv:1409.3199

  5. [13]

    LHCτ-rich tests of lepton-specific 2HDM for (g-2)µ

    E. J. Chun, Z. Kang, M. Takeuchi, and Y.-L. S. Tsai, “LHCτ-rich tests of lepton-specific 2HDM for (g-2)µ”,JHEP11(2015) 099,doi:10.1007/JHEP11(2015)099, arXiv:1507.08067

  6. [14]

    Theory and phenomenology of two-Higgs-doublet models

    G. C. Branco et al., “Theory and phenomenology of two-Higgs-doublet models”,Phys. Rept.516(2012) 1,doi:10.1016/j.physrep.2012.02.002,arXiv:1106.0034

  7. [15]

    Impersonating the Standard Model Higgs Boson: Alignment without Decoupling

    M. Carena, I. Low, N. R. Shah, and C. E. M. Wagner, “Impersonating the Standard Model Higgs Boson: Alignment without Decoupling”,JHEP04(2014) 015, doi:10.1007/JHEP04(2014)015,arXiv:1310.2248. 10

  8. [16]

    Supergauge invariant extension of the Higgs mechanism and a model for the electron and its neutrino

    P . Fayet, “Supergauge invariant extension of the Higgs mechanism and a model for the electron and its neutrino”,Nucl. Phys. B90(1975) 104, doi:10.1016/0550-3213(75)90636-7

  9. [17]

    Spontaneously broken supersymmetric theories of weak, electromagnetic and strong interactions

    P . Fayet, “Spontaneously broken supersymmetric theories of weak, electromagnetic and strong interactions”,Phys. Lett. B69(1977) 489, doi:10.1016/0370-2693(77)90852-8

  10. [18]

    Searches for additional Higgs bosons and for vector leptoquarks in ττfinal states in proton-proton collisions at √s= 13 TeV

    CMS Collaboration, “Searches for additional Higgs bosons and for vector leptoquarks in ττfinal states in proton-proton collisions at √s= 13 TeV”,JHEP07(2023) 073, doi:10.1007/JHEP07(2023)073,arXiv:2208.02717

  11. [19]

    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

  12. [20]

    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

  13. [21]

    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

  14. [22]

    HEPData record for this analysis

    “HEPData record for this analysis”, 2026.doi:10.17182/hepdata.166016

  15. [23]

    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

  16. [24]

    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

  17. [25]

    The CMS trigger system

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

  18. [26]

    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

  19. [27]

    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

  20. [28]

    Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √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

  21. [29]

    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

  22. [30]

    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. References 11

  23. [31]

    Performance of reconstruction and identification ofτleptons decaying to hadrons andν τ in pp collisions at √s=13 TeV

    CMS Collaboration, “Performance of reconstruction and identification ofτleptons decaying to hadrons andν τ in pp collisions at √s=13 TeV”,JINST13(2018) P10005, doi:10.1088/1748-0221/13/10/P10005,arXiv:1809.02816

  24. [32]

    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

  25. [33]

    Performance of missing transverse momentum reconstruction in proton-proton collisions at √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

  26. [34]

    Identification of hadronic tau lepton decays using a deep neural network

    CMS Collaboration, “Identification of hadronic tau lepton decays using a deep neural network”,JINST17(2022) P07023,doi:10.1088/1748-0221/17/07/P07023, arXiv:2201.08458

  27. [35]

    Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV

    CMS Collaboration, “Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV”,JINST13(2018) P05011, doi:10.1088/1748-0221/13/05/P05011,arXiv:1712.07158

  28. [36]

    Jet flavour classification using DeepJet

    E. Bols et al., “Jet flavour classification using DeepJet”,JINST15(2020) P12012, doi:10.1088/1748-0221/15/12/P12012,arXiv:2008.10519

  29. [37]

    Measurement of the Zγ ∗ →ττcross section in pp collisions at√s=13 TeV and validation ofτlepton analysis techniques

    CMS Collaboration, “Measurement of the Zγ ∗ →ττcross section in pp collisions at√s=13 TeV and validation ofτlepton analysis techniques”,Eur. Phys. J. C78(2018) 708,doi:10.1140/epjc/s10052-018-6146-9,arXiv:1801.03535

  30. [38]

    Reweighting with Boosted Decision Trees

    A. Rogozhnikov, “Reweighting with Boosted Decision Trees”,J. Phys. Conf. Ser.762 (2016) 012036,doi:10.1088/1742-6596/762/1/012036,arXiv:1608.05806

  31. [39]

    MadGraph 5: Going beyond

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

  32. [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

  33. [41]

    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

  34. [42]

    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

  35. [43]

    Hadronic top-quark pair-production with one jet and parton showering

    S. Alioli, S.-O. Moch, and P . Uwer, “Hadronic top-quark pair-production with one jet and parton showering”,JHEP01(2012) 137,doi:10.1007/JHEP01(2012)137, arXiv:1110.5251

  36. [44]

    Single-topt-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO

    R. Frederix, E. Re, and P . Torrielli, “Single-topt-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO”,JHEP09(2012) 130, doi:10.1007/JHEP09(2012)130,arXiv:1207.5391

  37. [45]

    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. 12

  38. [46]

    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

  39. [47]

    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

  40. [48]

    On the treatment of resonances in next-to-leading order calculations matched to a parton shower

    T. Je ˇzo and P . Nason, “On the treatment of resonances in next-to-leading order calculations matched to a parton shower”,JHEP12(2015) 065, doi:10.1007/JHEP12(2015)065,arXiv:1509.09071

  41. [49]

    Electroweak gauge boson production at hadron colliders throughO(α 2 s )

    K. Melnikov and F. Petriello, “Electroweak gauge boson production at hadron colliders throughO(α 2 s )”,Phys. Rev. D74(2006) 114017,doi:10.1103/PhysRevD.74.114017, arXiv:hep-ph/0609070

  42. [50]

    Top++: A program for the calculation of the top-pair cross-section at hadron colliders

    M. Czakon and A. Mitov, “Top++: A program for the calculation of the top-pair cross-section at hadron colliders”,Comput. Phys. Commun.185(2014) 2930, doi:10.1016/j.cpc.2014.06.021,arXiv:1112.5675

  43. [51]

    Top quark production

    N. Kidonakis, “Top quark production”, inProc. Helmholtz International Summer School on Physics of Heavy Quarks and Hadrons, p. 139. 2014.arXiv:1311.0283. doi:10.3204/DESY-PROC-2013-03/Kidonakis

  44. [52]

    Vector boson pair production at the LHC

    J. M. Campbell, R. K. Ellis, and C. Williams, “Vector boson pair production at the LHC”, JHEP07(2011) 018,doi:10.1007/JHEP07(2011)018,arXiv:1105.0020

  45. [53]

    W +W− production at hadron colliders in next to next to leading order QCD

    T. Gehrmann et al., “W +W− production at hadron colliders in next to next to leading order QCD”,Phys. Rev. Lett.113(2014) 212001, doi:10.1103/PhysRevLett.113.212001,arXiv:1408.5243

  46. [54]

    Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13 TeV

    CMS Collaboration, “Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at √s=13 TeV”,Eur. Phys. J. C81 (2021) 488,doi:10.1140/epjc/s10052-021-09200-x,arXiv:2103.04956

  47. [55]

    2HDECAY – A program for the calculation of electroweak one-loop corrections to Higgs decays in the Two-Higgs-Doublet Model including state-of-the-art QCD corrections

    M. Krause, M. M ¨uhlleitner, and M. Spira, “2HDECAY – A program for the calculation of electroweak one-loop corrections to Higgs decays in the Two-Higgs-Doublet Model including state-of-the-art QCD corrections”,Comput. Phys. Commun.246(2020) 106852, doi:10.1016/j.cpc.2019.08.0...

  48. [56]

    An introduction to PYTHIA 8.2

    T. Sj ¨ostrand et al., “An introduction to PYTHIA 8.2”,Comput. Phys. Commun.191(2015) 159,doi:10.1016/j.cpc.2015.01.024,arXiv:1410.3012

  49. [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

  50. [58]

    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

  51. [59]

    GEANT4—a simulation toolkit

    GEANT4 Collaboration, “GEANT4—a simulation toolkit”,Nucl. Instrum. Meth. A506 (2003) 250,doi:10.1016/S0168-9002(03)01368-8. References 13

  52. [60]

    Measurements of inclusive W and Z cross sections in pp collisions at √s=7 TeV

    CMS Collaboration, “Measurements of inclusive W and Z cross sections in pp collisions at √s=7 TeV”,JHEP01(2011) 080,doi:10.1007/JHEP01(2011)080, arXiv:1012.2466

  53. [61]

    Fitting using finite Monte Carlo samples

    R. J. Barlow and C. Beeston, “Fitting using finite Monte Carlo samples”,Comput. Phys. Commun.77(1993) 219,doi:10.1016/0010-4655(93)90005-W

  54. [62]

    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

  55. [63]

    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]

  56. [64]

    Confidence level computation for combining searches with small statistics

    T. Junk, “Confidence level computation for combining searches with small statistics”, Nucl. Instrum. Meth. A434(1999) 435,doi:10.1016/S0168-9002(99)00498-2, arXiv:hep-ex/9902006

  57. [65]

    Presentation of search results: The CL s technique

    A. L. Read, “Presentation of search results: The CL s technique”,J. Phys. G28(2002) 2693, doi:10.1088/0954-3899/28/10/313

  58. [66]

    HiggsTools: BSM scalar phenomenology with new versions of HiggsBounds and HiggsSignals

    H. Bahl et al., “HiggsTools: BSM scalar phenomenology with new versions of HiggsBounds and HiggsSignals”,Comput. Phys. Commun.291(2023) 108803, doi:10.1016/j.cpc.2023.108803,arXiv:2210.09332. 14 15 A The CMS Collaboration Yerevan Physics Institute, Yerevan, Armenia A. Hayrapet...

Pith tools

Reviewed May 19, 2026 · model on record in the stance chip above.