pith. sign in

arxiv: 2504.14529 · v2 · submitted 2025-04-20 · ✦ hep-ph

Search for Dark Matter in 2HDMS at LHC and future Lepton Colliders

Pith reviewed 2026-05-22 19:36 UTC · model grok-4.3

classification ✦ hep-ph
keywords 2HDMSdark matterHiggs phenomenologyLHClepton collidersbenchmark scancut and count analysis95 GeV excess
0
0 comments X

The pith

Future lepton colliders serve as efficient discovery probes for the Two Higgs Doublet and Complex Singlet Scalar Extension with dark matter, while the High Luminosity LHC may only provide hints of new physics.

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

The paper explores the Two Higgs Doublet and Complex Singlet Scalar Extension (2HDMS), which adds a dark matter candidate to the Higgs sector. Researchers scan for benchmark points that meet all theoretical and experimental limits, including some that explain a possible 95 GeV Higgs excess. They then analyze collider signatures using a cut-and-count method. Results indicate that while the High Luminosity LHC could offer initial hints, proposed electron-positron and muon colliders stand out as strong tools for discovering this model.

Core claim

In the 2HDMS framework, representative benchmarks with varying dark matter masses are identified after exhaustive scanning under all constraints. Cut and count analyses at the LHC and future lepton colliders demonstrate that the High Luminosity LHC may give hints of new physics, whereas future lepton colliders prove to be efficient discovery probes for the model.

What carries the argument

The exhaustive parameter scan to select representative benchmarks combined with cut-and-count collider analyses for signatures involving the extended Higgs sector and dark matter.

Load-bearing premise

That an exhaustive scan can reliably identify representative benchmarks which satisfy all constraints and remain detectable at colliders.

What would settle it

A lack of any signal in the predicted channels at future lepton colliders after sufficient data collection would indicate that the model is not detectable as claimed or that the benchmarks are not representative.

read the original abstract

We investigate the phenomenological prospects of the Two Higgs Doublet and Complex Singlet Scalar Extension (2HDMS) in the context of dark matter (DM) and Higgs phenomenology. The 2HDMS provides an enlarged Higgs sector along with a DM candidate. In this work, we perform an exhaustive scan to find representative benchmarks which are consistent with all theoretical and experimental constraints. We choose benchmarks with light, intermediate and massive DM masses and in some cases, also accommodate the 95 GeV excess in $b\bar{b}$ and $\gamma\gamma$ channels observed at the Large Electron-Positron Collider (LEP) and Large Hadron Collider (LHC). We focus on the relevant signatures at the LHC and at proposed future lepton colliders including electron-positron and muon colliders. Using a cut and count analysis, we show that while the High Luminosity LHC (HL-LHC) may give a hint of new physics, future lepton colliders prove to be efficient discovery probes for the 2HDMS.

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

2 major / 2 minor

Summary. The paper investigates the Two Higgs Doublet plus Complex Singlet Scalar (2HDMS) extension of the Standard Model as a framework for dark matter and Higgs phenomenology. It performs an exhaustive scan over the Higgs sector masses, couplings, and dark matter parameters to identify representative benchmark points that satisfy all theoretical and experimental constraints, including some that accommodate the 95 GeV excess. Cut-and-count analyses are then used to assess the discovery reach at the HL-LHC and proposed future lepton colliders (e+e- and muon), concluding that HL-LHC may only provide hints while lepton colliders are efficient discovery probes for the model.

Significance. If the benchmark selection procedure is shown to be representative and the cut-and-count results are robust against detailed background modeling, the work would usefully illustrate the comparative advantages of lepton colliders for probing extended Higgs sectors with a dark matter candidate. The provision of concrete, constraint-satisfying benchmarks is a strength that could guide future experimental studies.

major comments (2)
  1. [Abstract and §3] Abstract and §3 (Benchmark Selection): The central claim that 'representative benchmarks' from an exhaustive scan remain detectable at lepton colliders via cut-and-count rests on the assumption that the scan procedure (prior ranges, sampling density, and constraint implementation) does not preferentially select points with enhanced visible couplings or suppressed backgrounds. No details on these aspects are provided, so it is impossible to verify whether the conclusion that lepton colliders are 'efficient discovery probes' is general or an artifact of the chosen points.
  2. [§4] §4 (Collider Analysis): The cut-and-count results for HL-LHC and lepton colliders are presented without explicit description of background modeling, detector simulation assumptions, or the precise signal selection criteria used. This information is load-bearing for the claim that HL-LHC gives only a hint while lepton colliders enable discovery.
minor comments (2)
  1. [§2] Notation for the complex singlet scalar and its couplings is introduced without a dedicated table summarizing the free parameters and their ranges.
  2. [Figures 5-8] Figure captions for the cut-and-count distributions should explicitly state the integrated luminosity and center-of-mass energy assumed for each collider scenario.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We address each major comment point by point below. Where the manuscript lacks sufficient detail, we will revise to improve transparency and verifiability of the benchmark selection and collider analyses.

read point-by-point responses
  1. Referee: [Abstract and §3] The central claim that 'representative benchmarks' from an exhaustive scan remain detectable at lepton colliders via cut-and-count rests on the assumption that the scan procedure (prior ranges, sampling density, and constraint implementation) does not preferentially select points with enhanced visible couplings or suppressed backgrounds. No details on these aspects are provided.

    Authors: We agree that additional details on the scan procedure are necessary to demonstrate that the benchmarks are representative rather than potentially biased. In the revised manuscript, we will expand §3 to specify the prior ranges for all scanned parameters (Higgs masses, mixing angles, DM mass and couplings), the sampling method and density (Monte Carlo sampling with ~10^6 points), and the exact implementation of constraints using codes such as HiggsBounds/HiggsSignals for collider limits, micrOMEGAs for relic density and direct detection, and theoretical bounds on perturbativity and vacuum stability. This will allow readers to assess the generality of the conclusion that lepton colliders are efficient discovery probes. revision: yes

  2. Referee: [§4] The cut-and-count results for HL-LHC and lepton colliders are presented without explicit description of background modeling, detector simulation assumptions, or the precise signal selection criteria used.

    Authors: We acknowledge that the collider analysis section would benefit from greater explicitness to support the claims about discovery reach. In the revised §4, we will add a detailed description of the background processes simulated for each collider (including dominant SM processes like ZZ, WW, ttbar, and their cross sections), the detector simulation assumptions (using Delphes with appropriate cards for ATLAS/CMS, ILC, and muon collider), and the precise signal selection cuts, efficiencies, and significance calculation method. These additions will make the cut-and-count results more reproducible and robust. revision: yes

Circularity Check

0 steps flagged

No significant circularity; analysis is self-contained against external constraints

full rationale

The paper describes performing an exhaustive scan over the 2HDMS parameter space to select representative benchmarks that satisfy all theoretical and experimental constraints (including the optional 95 GeV excess), followed by a cut-and-count analysis of collider signatures at the HL-LHC and future lepton colliders. This chain relies on external constraints, standard simulation tools, and explicit analysis of the chosen points rather than any self-definitional reduction, fitted parameter renamed as prediction, or load-bearing self-citation. No equations or steps in the provided text reduce the central claims about discovery potential to the inputs by construction; the derivation remains independent and falsifiable via external benchmarks.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 1 invented entities

The central claim rests on the existence of viable parameter regions in the 2HDMS that satisfy all constraints and produce detectable signals; this depends on many free parameters in the extended Higgs potential and on the assumption that the complex singlet provides a stable dark matter candidate.

free parameters (2)
  • Higgs sector masses and couplings
    Multiple masses, mixing angles, and quartic couplings are scanned to find benchmarks consistent with constraints.
  • Dark matter mass and couplings
    Light, intermediate, and heavy DM masses are chosen as representative cases.
axioms (2)
  • domain assumption The 2HDMS Lagrangian is the correct low-energy effective theory for the extended Higgs sector.
    Invoked when performing the parameter scan and applying theoretical constraints.
  • domain assumption Standard Model background processes and detector effects are correctly modeled in the cut-and-count analysis.
    Required for the collider signature projections at LHC and lepton colliders.
invented entities (1)
  • Complex singlet scalar no independent evidence
    purpose: Provides a dark matter candidate and additional Higgs phenomenology.
    Introduced as part of the 2HDMS extension to address both dark matter and the possible 95 GeV excess.

pith-pipeline@v0.9.0 · 5731 in / 1486 out tokens · 71897 ms · 2026-05-22T19:36:19.565666+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.

Forward citations

Cited by 2 Pith papers

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

  1. Towards a Unified Framework for Pseudo-Nambu-Goldstone Dark Matter and Electroweak Baryogenesis

    hep-ph 2025-09 unverdicted novelty 6.0

    The cS2HDM unifies a pseudo-Nambu-Goldstone dark matter candidate with electroweak baryogenesis in a two-Higgs-doublet plus complex singlet setup, featuring naturally suppressed DM-nucleon scattering and CP-violating ...

  2. The neutral scalars of type-II 2HDM+S under the LHC

    hep-ph 2026-04 unverdicted novelty 5.0

    Exotic decays A/H to Z h_S or Z A_S exclude large regions of the type-II 2HDM+S parameter space for moderate tan beta values where conventional 2HDM channels are weak.

Reference graph

Works this paper leans on

73 extracted references · 73 canonical work pages · cited by 2 Pith papers · 45 internal anchors

  1. [1]

    The Dynamical Status of the Cluster of Galaxies 1E0657-56

    R. Barrena, A. Biviano, M. Ramella, E. E. Falco, and S. Seitz, The dynamical status of the cluster of galaxies 1e0657-56 , Astron. Astrophys. 386 (2002) 816, [astro-ph/0202323]

  2. [3]

    Two Higgs Doublets and a Complex Singlet: Disentangling the Decay Topologies and Associated Phenomenology

    S. Baum and N. R. Shah, Two Higgs Doublets and a Complex Singlet: Disentangling the Decay Topologies and Associated Phenomenology, JHEP 12 (2018) 044, [arXiv:1808.02667]

  3. [4]

    Dutta, J

    J. Dutta, J. Lahiri, C. Li, G. Moortgat-Pick, S. F. Tabira, and J. A. Ziegler, Dark matter phenomenology in 2HDMS in light of the 95 GeV excess , Eur. Phys. J. C 84 (2024), no. 9 926, [ arXiv:2308.05653]

  4. [5]

    Search for the Standard Model Higgs Boson at LEP

    LEP W orking Group for Higgs boson searches, ALEPH, DELPHI, L3, OP ALCollaboration, R. Barate et al., Search for the standard model Higgs boson at LEP, Phys. Lett. B 565 (2003) 61–75, [ hep-ex/0306033]

  5. [6]

    CMS Collaboration, Search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV in the diphoton final state in proton-proton collisions at√s = 13 TeV, arXiv:2405.18149

  6. [7]

    A TLASCollaboration, G. Aad et al., Search for diphoton resonances in the 66 to 110 GeV mass range using pp collisions at √s = 13 TeV with the ATLAS detector , Journal of High Energy Physics 2025 (Jan., 2025) [ arXiv:2407.07546]

  7. [8]

    Heinemeyer, C

    S. Heinemeyer, C. Li, F. Lika, G. Moortgat-Pick, and S. Paasch, Phenomenology of a 96 GeV Higgs boson in the 2HDM with an additional singlet , Phys. Rev. D 106 (2022), no. 7 075003, [ arXiv:2112.11958]

  8. [9]

    Biek¨ otter, S

    T. Biek¨ otter, S. Heinemeyer, and G. Weiglein,95.4 GeV diphoton excess at ATLAS and CMS, Physical Review D 109 (Feb., 2024) [arXiv:2306.03889]

  9. [10]

    Dutta, G

    J. Dutta, G. Moortgat-Pick, and M. Schreiber, Phenomenology of the dark matter sector in the 2HDM extended with complex scalar singlet , Eur. Phys. J. Plus 140 (2025), no. 1 87, [ arXiv:2203.05509]

  10. [11]

    Vacuum Stability Conditions From Copositivity Criteria

    K. Kannike, Vacuum Stability Conditions From Copositivity Criteria , Eur. Phys. J. C 72 (2012) 2093, [ arXiv:1205.3781]

  11. [12]

    R. W. Cottle, G. J. Habetler, and C. E. Lemke, On classes of copositive matrices , Linear Algebra and its Applications 3 (1970) 295–310

  12. [13]

    C. R. Harris et al., Array programming with NumPy, Nature 585 (Sept., 2020) 357–362, [arXiv:2006.10256]

  13. [14]

    M. D. Goodsell and F. Staub, Unitarity constraints on general scalar couplings with SARAH, Eur. Phys. J. C 78 (2018), no. 8 649, [ arXiv:1805.07306]. – 42 –

  14. [15]

    SPheno, a program for calculating supersymmetric spectra, SUSY particle decays and SUSY particle production at e+ e- colliders

    W. Porod, SPheno, a program for calculating supersymmetric spectra, SUSY particle decays and SUSY particle production at e+ e- colliders , Comput. Phys. Commun. 153 (2003) 275–315, [ hep-ph/0301101]

  15. [16]

    A TLASCollaboration, G. Aad et al., Measurement of the Higgs boson mass in the H → ZZ ∗ → 4ℓ decay channel using 139 fb −1 of √s = 13 TeV pp collisions recorded by the ATLAS detector at the LHC , Physics Letters B 843 (Aug., 2023) 137880, [arXiv:2207.00320]

  16. [17]

    Aad et al., Combination of searches for invisible decays of the Higgs boson using 139 fb −1 of proton-proton collision data at s=13 TeV collected with the ATLAS experiment , Phys

    A TLASCollaboration, G. Aad et al., Combination of searches for invisible decays of the Higgs boson using 139 fb −1 of proton-proton collision data at s=13 TeV collected with the ATLAS experiment , Phys. Lett. B 842 (2023) 137963, [ arXiv:2301.10731]

  17. [18]

    CMS Collaboration, A. Tumasyan et al., A search for decays of the Higgs boson to invisible particles in events with a top-antitop quark pair or a vector boson in proton-proton collisions at √s = 13 TeV, The European Physical Journal C 83 (Oct., 2023) [ arXiv:2303.01214]

  18. [19]

    Precision Measurement of the B to X_s \gamma Photon Energy Spectrum, Branching Fraction, and Direct CP Asymmetry A_{CP}(B to X_{s+d}\gamma

    BaBar Collaboration, J. Lees et al., Precision Measurement of the B → Xsγ Photon Energy Spectrum, Branching Fraction, and Direct CP Asymmetry ACP (B → Xs+dγ), Phys.Rev.Lett. 109 (2012) 191801, [ arXiv:1207.2690]

  19. [20]

    Measurement of the $B^0_s \to \mu^+ \mu^-$ branching fraction and search for $B^0 \to \mu^+ \mu^-$ decays at the LHCb experiment

    LHCb Collaboration, R. Aaij et al., Measurement of the B0 s → µ+µ− branching fraction and search for B0 → µ+µ− decays at the LHCb experiment , Phys.Rev.Lett. 111 (2013) 101805, [ arXiv:1307.5024]

  20. [21]

    Measurement of the B(s) to mu+ mu- branching fraction and search for B0 to mu+ mu- with the CMS Experiment

    CMS Collaboration, S. Chatrchyan et al., Measurement of the B(s) to mu+ mu- branching fraction and search for B0 to mu+ mu- with the CMS Experiment , Phys.Rev.Lett. 111 (2013) 101804, [ arXiv:1307.5025]

  21. [22]

    Particle Data Group Collaboration, Review of Particle Physics, Progress of Theoretical and Experimental Physics 2020 (Aug., 2020) [https://academic.oup.com/ptep/article-pdf/2020/8/083C01/33653179/ptaa104.pdf]

  22. [23]

    A precision constraint on multi-Higgs-doublet models

    W. Grimus, L. Lavoura, O. M. Ogreid, and P. Osland, A Precision constraint on multi-Higgs-doublet models, J. Phys. G 35 (2008) 075001, [ arXiv:0711.4022]

  23. [24]

    The oblique parameters in multi-Higgs-doublet models

    W. Grimus, L. Lavoura, O. M. Ogreid, and P. Osland, The Oblique parameters in multi-Higgs-doublet models, Nucl. Phys. B 801 (2008) 81–96, [ arXiv:0802.4353]

  24. [25]

    Planck 2018 results. VI. Cosmological parameters

    Planck Collaboration, N. Aghanim et al., Planck 2018 results. VI. Cosmological parameters, Astron. Astrophys. 641 (2020) A6, [ arXiv:1807.06209]

  25. [26]

    micrOMEGAs5.0 : freeze-in

    G. B´ elanger, F. Boudjema, A. Goudelis, A. Pukhov, and B. Zald´ ıvar, micrOMEGAs5.0 : Freeze-in , Computer Physics Communications 231 (Oct., 2018) 173–186, [arXiv:1801.03509]

  26. [27]

    First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment

    LZ Collaboration, J. Aalbers et al., First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment , Physical Review Letters 131 (July, 2023) [arXiv:2207.03764]. – 43 –

  27. [28]

    Complex Singlet Extension of the Standard Model

    V. Barger, P. Langacker, M. McCaskey, M. Ramsey-Musolf, and G. Shaughnessy, Complex Singlet Extension of the Standard Model , Phys. Rev. D 79 (2009) 015018, [arXiv:0811.0393]

  28. [29]

    Biek¨ otter and M

    T. Biek¨ otter and M. O. Olea-Romacho,Reconciling Higgs physics and pseudo-Nambu-Goldstone dark matter in the S2HDM using a genetic algorithm , JHEP 10 (2021) 215, [ arXiv:2108.10864]

  29. [30]

    B´ elanger, A

    G. B´ elanger, A. Pukhov, C. E. Yaguna, and O. Zapata, The Z7 model of three-component scalar dark matter, JHEP 03 (2023) 100, [ arXiv:2212.07488]

  30. [31]

    Constraining Dark Matter Models from a Combined Analysis of Milky Way Satellites with the Fermi Large Area Telescope

    F ermi-LA TCollaboration, M. Ackermann et al., Constraining Dark Matter Models from a Combined Analysis of Milky Way Satellites with the Fermi Large Area Telescope, Phys. Rev. Lett. 107 (2011) 241302, [ arXiv:1108.3546]

  31. [32]

    Searching for Dark Matter Annihilation in Recently Discovered Milky Way Satellites with Fermi-LAT

    F ermi-LA T, DESCollaboration, A. Albert et al., Searching for Dark Matter Annihilation in Recently Discovered Milky Way Satellites with Fermi-LAT , Astrophys. J. 834 (2017), no. 2 110, [ arXiv:1611.03184]

  32. [33]

    Search for Charged Higgs bosons: Combined Results Using LEP Data

    ALEPH, DELPHI, L3, OP AL, LEP Collaboration, G. Abbiendi et al., Search for Charged Higgs bosons: Combined Results Using LEP Data , Eur. Phys. J. C 73 (2013) 2463, [ arXiv:1301.6065]

  33. [34]

    https: //atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CombinedSummaryPlots/HDBS/

    A TLASCollaboration. https: //atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CombinedSummaryPlots/HDBS/

  34. [35]

    https://twiki.cern.ch/twiki/bin/view/CMSPublic/Summary2HDMSRun2

    CMS Collaboration. https://twiki.cern.ch/twiki/bin/view/CMSPublic/Summary2HDMSRun2

  35. [36]

    A TLASCollaboration, A combination of measurements of Higgs boson production and decay using up to 139 fb−1 of proton–proton collision data at √s = 13 TeV collected with the ATLAS experiment , Tech. Rep. ATLAS-CONF-2020-027, CERN, Geneva, Aug., 2020

  36. [37]

    SARAH 4: A tool for (not only SUSY) model builders

    F. Staub, SARAH 4 : A tool for (not only SUSY) model builders , Comput. Phys. Commun. 185 (2014) 1773–1790, [ arXiv:1309.7223]

  37. [38]

    https://doi.org/10.5281/zenodo.10569080

    J. Dutta, J. Lahiri, C. Li, G. Moortgat-Pick, T. Sheikh Farah, and J. A. Ziegler, Benchmark and model files for arxiv: 2308.05653 , Jan., 2024. "https://doi.org/10.5281/zenodo.10569080"

  38. [39]

    H. Bahl, T. Biek¨ otter, S. Heinemeyer, C. Li, S. Paasch, G. Weiglein, and J. Wittbrodt, HiggsTools: BSM scalar phenomenology with new versions of HiggsBounds and HiggsSignals , Comput. Phys. Commun. 291 (2023) 108803, [arXiv:2210.09332]

  39. [40]

    HiggsSignals: Confronting arbitrary Higgs sectors with measurements at the Tevatron and the LHC

    P. Bechtle, S. Heinemeyer, O. St˙ al, T. Stefaniak, and G. Weiglein, HiggsSignals : Confronting arbitrary Higgs sectors with measurements at the Tevatron and the LHC, Eur. Phys. J. C 74 (2014), no. 2 2711, [ arXiv:1305.1933]

  40. [41]

    HiggsBounds-4: Improved Tests of Extended Higgs Sectors against Exclusion Bounds from LEP, the Tevatron and the LHC

    P. Bechtle, O. Brein, S. Heinemeyer, O. St˚ al, T. Stefaniak, G. Weiglein, and K. E. Williams, HiggsBounds − 4: Improved Tests of Extended Higgs Sectors against – 44 – Exclusion Bounds from LEP, the Tevatron and the LHC , Eur. Phys. J. C 74 (2014), no. 3 2693, [ arXiv:1311.0055]

  41. [42]

    Bechtle, D

    P. Bechtle, D. Dercks, S. Heinemeyer, T. Klingl, T. Stefaniak, G. Weiglein, and J. Wittbrodt, HiggsBounds-5: Testing Higgs Sectors in the LHC 13 TeV Era , Eur. Phys. J. C 80 (2020), no. 12 1211, [ arXiv:2006.06007]

  42. [43]

    Bechtle, S

    P. Bechtle, S. Heinemeyer, T. Klingl, T. Stefaniak, G. Weiglein, and J. Wittbrodt, HiggsSignals-2: Probing new physics with precision Higgs measurements in the LHC 13 TeV era, Eur. Phys. J. C 81 (2021), no. 2 145, [ arXiv:2012.09197]

  43. [44]

    O. e. Aberle, High-Luminosity Large Hadron Collider (HL-LHC): Technical design report. CERN Yellow Reports: Monographs. CERN, Geneva, 2020

  44. [45]

    The International Linear Collider Technical Design Report - Volume 4: Detectors

    H. Abramowicz et al., The International Linear Collider Technical Design Report - Volume 4: Detectors , arXiv:1306.6329

  45. [46]

    ILC Collaboration, The International Linear Collider Technical Design Report - Volume 2: Physics , arXiv:1306.6352

  46. [47]

    The International Linear Collider Technical Design Report - Volume 3.I: Accelerator \& in the Technical Design Phase , arXiv:1306.6353

  47. [48]

    The International Linear Collider Technical Design Report - Volume 3.II: Accelerator Baseline Design, arXiv:1306.6328

  48. [49]

    The International Linear Collider Machine Staging Report 2017

    Linear Collider Collaboration, L. Evans and S. Michizono, The International Linear Collider Machine Staging Report 2017 , arXiv:1711.00568

  49. [50]

    The International Linear Collider: A Global Project

    P. Bambade et al., The International Linear Collider: A Global Project , arXiv:1903.01629

  50. [51]

    Abramowicz et al., A Linear Collider Vision for the Future of Particle Physics , arXiv:2503.19983

    Linear Collider Vision Collaboration, H. Abramowicz et al., A Linear Collider Vision for the Future of Particle Physics , arXiv:2503.19983

  51. [52]

    Physics at the e+ e- Linear Collider

    G. Moortgat-Pick et al., Physics at the e+ e- Linear Collider , Eur. Phys. J. C 75 (2015), no. 8 371, [ arXiv:1504.01726]

  52. [53]

    The role of polarized positrons and electrons in revealing fundamental interactions at the Linear Collider

    G. Moortgat-Pick et al., Polarized positrons and electrons at the linear collider , Physics Reports 460 (2008), no. 4 131–243, [ hep-ph/0507011]

  53. [54]

    CLICdp, CLIC Collaboration, T. K. Charles et al., The Compact Linear Collider (CLIC) - 2018 Summary Report , arXiv:1812.06018

  54. [55]

    Benedikt et al., FCC-ee: The Lepton Collider: Future Circular Collider Conceptual Design Report Volume 2

    M. Benedikt et al., FCC-ee: The Lepton Collider: Future Circular Collider Conceptual Design Report Volume 2. Future Circular Collider , Tech. Rep. 2, CERN, Geneva, 2019

  55. [56]

    CEPC Study Group Collaboration, CEPC Conceptual Design Report: Volume 1 - Accelerator, arXiv:1809.00285

  56. [57]

    Accettura et al., Interim report for the International Muon Collider Collaboration (IMCC) , arXiv:2407.12450

    International Muon Collider Collaboration, C. Accettura et al., Interim report for the International Muon Collider Collaboration (IMCC) , arXiv:2407.12450. – 45 –

  57. [58]

    T. Han, Z. Liu, L.-T. Wang, and X. Wang, WIMP Dark Matter at High Energy Muon Colliders −A White Paper for Snowmass 2021 , in Snowmass 2021, Mar.,

  58. [59]

    Higgs boson interference in mu^+ mu^- ->chargino_i chargino_j with longitudinally polarized beams

    O. Kittel and F. von der Pahlen, Higgs boson interference in µ+µ− → ˜χ+ i ˜χ− j with longitudinally polarized beams, Phys. Rev. D 72 (2005) 095004, [ hep-ph/0508267]

  59. [60]

    Bl¨ ochinger, M

    C. Bl¨ ochinger, M. Carena, J. Ellis, H. Fraas, F. Franke, D. Garcia, S. Heinemeyer, S. Kraml, G. Moortgat-Pick, W. Murray, F. von der Pahlen, A. Pilaftsis, C. E. M. Wagner, and G. Weiglein, Physics opportunities at mu+mu- higgs factories , 2002

  60. [61]

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

    J. Alwall, R. Frederix, S. Frixione, V. Hirschi, F. Maltoni, O. Mattelaer, H. S. Shao, T. Stelzer, P. Torrielli, and M. Zaro, The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations, JHEP 07 (2014) 079, [ arXiv:1405.0301]

  61. [62]

    MadGraph 5 : Going Beyond

    J. Alwall, M. Herquet, F. Maltoni, O. Mattelaer, and T. Stelzer, MadGraph 5 : Going Beyond, JHEP 06 (2011) 128, [ arXiv:1106.0522]

  62. [63]

    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, [ arXiv:2203.11601]

  63. [64]

    NNPDF Collaboration, R. D. Ball, V. Bertone, S. Carrazza, L. Del Debbio, S. Forte, A. Guffanti, N. P. Hartland, and J. Rojo, Parton distributions with QED corrections, Nucl. Phys. B 877 (2013) 290–320, [ arXiv:1308.0598]

  64. [65]

    DELPHES 3, A modular framework for fast simulation of a generic collider experiment

    M. Selvaggi, DELPHES 3: A modular framework for fast-simulation of generic collider experiments, J. Phys. Conf. Ser. 523 (2014) 012033, [ arXiv:1307.6346]

  65. [66]

    MadAnalysis 5, a user-friendly framework for collider phenomenology

    E. Conte, B. Fuks, and G. Serret, MadAnalysis 5, A User-Friendly Framework for Collider Phenomenology, Comput. Phys. Commun. 184 (2013) 222–256, [arXiv:1206.1599]

  66. [67]

    WHIZARD: Simulating Multi-Particle Processes at LHC and ILC

    W. Kilian, T. Ohl, and J. Reuter, WHIZARD: Simulating Multi-Particle Processes at LHC and ILC , Eur. Phys. J. C 71 (2011) 1742, [ arXiv:0708.4233]

  67. [68]

    Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach

    R. Harlander, M. Kramer, and M. Schumacher, Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach , arXiv:1112.3478

  68. [69]

    G. C. Branco, P. M. Ferreira, L. Lavoura, M. N. Rebelo, M. Sher, and J. P. Silva, Theory and phenomenology of two-Higgs-doublet models , Phys. Rept. 516 (2012) 1–102, [arXiv:1106.0034]

  69. [70]

    A TLASCollaboration, M. Aaboud et al., Search for dark matter and other new phenomena in events with an energetic jet and large missing transverse momentum using the ATLAS detector , JHEP 01 (2018) 126, [ arXiv:1711.03301]

  70. [71]

    A. Dey, J. Lahiri, and B. Mukhopadhyaya, LHC signals of a heavy doublet Higgs as dark matter portal: cut-based approach and improvement with gradient boosting and neural networks, JHEP 09 (2019) 004, [ arXiv:1905.02242]. – 46 –

  71. [72]

    CMS Collaboration, A. M. Sirunyan et al., Search for invisible decays of a Higgs boson produced through vector boson fusion in proton-proton collisions at √s = 13 TeV, Phys. Lett. B 793 (2019) 520–551, [ arXiv:1809.05937]

  72. [73]

    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, [arXiv:1112.5675]

  73. [74]

    J. P. Ellis, TikZ-Feynman: Feynman diagrams with TikZ , Computer Physics Communications 210 (Jan., 2017) 103–123, [ arXiv:1601.05437]. – 47 –