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arxiv: 2605.13336 · v1 · submitted 2026-05-13 · ✦ hep-ph

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Probing Boosted Light Scalars in the Type-I 2HDM

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Pith reviewed 2026-05-14 18:24 UTC · model grok-4.3

classification ✦ hep-ph
keywords Type-I 2HDMlight scalarsboosted fat-jetsHL-LHCelectroweak productiondouble-b jet taggingscalar mass hierarchy
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The pith

Tagging boosted double-b fat-jets from light scalars paired with gauge bosons can exclude heavy scalars up to 540 GeV at the HL-LHC in Type-I 2HDM.

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

The paper demonstrates that in the Type-I two-Higgs-doublet model, light scalars between 30 and 70 GeV can be produced electroweakly alongside heavier scalars or pseudoscalars that decay into them, yielding boosted light scalars whose b-quark pairs form identifiable fat-jets. Pairing the fat-jet tag with a standard-model gauge boson creates a searchable signature that reaches parameter regions missed by existing strategies relying on Higgs decays or direct b b-bar production. This approach yields 2 sigma exclusion of heavy scalars up to roughly 540 GeV at the high-luminosity LHC with 3000 inverse femtobarns and 365 GeV at the current LHC with 300 inverse femtobarns. The same method also supports model-independent resonance reconstruction, showing the signature remains useful even without full model assumptions.

Core claim

Electroweak production of a light scalar h together with a heavy pseudoscalar A or charged Higgs H±, followed by A or H± decaying to h plus a gauge boson, produces boosted h particles that decay to b b-bar and are reconstructed as a single fat-jet containing two b-subjets. Tagging this boosted double-b fat-jet signature in association with a standard-model gauge boson therefore probes large parts of the Type-I 2HDM parameter space for hierarchical scalar masses, delivering 2 sigma exclusion reaches for the heavy states up to approximately 540 GeV at the HL-LHC with 3000 fb^{-1} for light scalar masses in the 30-70 GeV window.

What carries the argument

The boosted double-b fat-jet (J_bb) formed by the two b-subjets from the decay of a light scalar h, tagged together with an accompanying SM gauge boson.

Load-bearing premise

The light scalar must decay predominantly to b b-bar with high branching ratio, the fat-jet tagging efficiency must stay high, and standard-model backgrounds must remain controllable at the quoted luminosities.

What would settle it

Absence of excess events above background in the J_bb plus gauge-boson channel at the HL-LHC for heavy-scalar masses near 500 GeV with 3000 fb^{-1} would falsify the projected 2 sigma exclusion reach.

read the original abstract

In the Type-I two-Higgs Doublet Model (2HDM), the additional scalars may be light ($\lesssim 100$ GeV) without conflicting with experimental constraints from LHC searches or from flavour observables. So far, the studies of light scalars at the LHC have been limited to exploring non-standard decays of the Standard Model (SM) Higgs boson or via $b\bar b$ associated production followed by leptonic decays of the light scalar. A light scalar in Type-I 2HDM can evade these search strategies due to its potentially tiny coupling to the SM Higgs boson and its suppressed coupling to quarks. In this work, we have studied electroweak production of a light scalar ($h$) in association with heavy pseudoscalar $A$ or charged Higgs $H^\pm$, which further decays into $h$, resulting in a multi-$h$ final state, where $h$ is boosted due to its lightness. The decay of the boosted $h$ into $b\bar b$ can be reconstructed within a fat-jet containing a pair of $b$-subjets. We find that tagging such a `boosted double-$b$ fat-jet ($J_{bb}$)' signature in association with a SM gauge boson provides an excellent probe of the Type-I 2HDM for hierarchical scalar spectra. Using multiple light mass $M_h$ benchmarks, we demonstrate that such analysis can explore a large region of the parameter space, with the $2\sigma$ exclusion reach for the heavy scalars extending up to $\sim 540$ GeV ($\sim$ 365 GeV) at the HL-LHC with 3000 fb$^{-1}$ (LHC with 300 fb$^{-1}$) luminosity for light scalar masses in the range $30$--$70$ GeV. Furthermore, we show that significant sensitivity and even resonance reconstruction can be achieved within a model-independent framework, highlighting the robustness of this search strategy.

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

3 major / 1 minor

Summary. The paper proposes using electroweak production of a light scalar h (30-70 GeV) in association with heavy A or H± in the Type-I 2HDM, where the heavy states decay to h plus a gauge boson, yielding a boosted h reconstructed as a double-b fat-jet (J_bb) plus SM gauge boson. It claims this signature probes hierarchical spectra with 2σ exclusion reaches for heavy scalars up to ~540 GeV at HL-LHC (3000 fb^{-1}) and ~365 GeV at LHC (300 fb^{-1}), and demonstrates sensitivity in a model-independent framework.

Significance. If the analysis holds, the work provides a new channel for light scalars in Type-I 2HDM where traditional b-associated or SM-Higgs-decay searches are limited by suppressed couplings. The boosted J_bb tagging approach for multi-Higgs final states could meaningfully extend LHC sensitivity to hierarchical spectra.

major comments (3)
  1. [Abstract] Abstract: the quoted 2σ exclusion reaches (~540 GeV at HL-LHC) are presented without any reported details on background modeling for V + multi-jet processes, systematic uncertainties on the J_bb tagging working point, or validation of tagging efficiency, which directly limits support for the numerical claims.
  2. [Model and benchmarks] Model section: in Type-I 2HDM the light scalar's fermion couplings are scaled by a mixing factor (cos(β-α) or equivalent), which can suppress the partial width to bb relative to gg or ττ; the reach estimates assume BR(h→bb) remains high enough for the signal yield, but no explicit branching-ratio calculations or scans over the mixing angle are shown for the benchmarks.
  3. [Analysis and results] Analysis and results: the projected reaches rely on standard Monte Carlo simulations of signal and background without data-driven validation or discussion of how high-pT V + jets backgrounds are controlled after the fat-jet tagging, making the precise luminosity-dependent numbers sensitive to unquantified assumptions.
minor comments (1)
  1. [Introduction] The notation J_bb for the boosted double-b fat-jet is introduced in the abstract but would benefit from an explicit definition and efficiency parametrization in the methods section for clarity.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the constructive and detailed comments. We have addressed each major point below, providing clarifications and indicating where revisions will be incorporated to strengthen the manuscript.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the quoted 2σ exclusion reaches (~540 GeV at HL-LHC) are presented without any reported details on background modeling for V + multi-jet processes, systematic uncertainties on the J_bb tagging working point, or validation of tagging efficiency, which directly limits support for the numerical claims.

    Authors: We agree that the abstract is concise and omits technical details on background modeling, systematic uncertainties, and tagging validation. These elements are presented in the Analysis and Results sections, where we describe the Monte Carlo generation of V + jets backgrounds, the J_bb tagging algorithm performance (efficiency and mistag rates derived from simulation), and basic systematic variations. To better support the quoted reaches, we will revise the abstract to include a brief reference to the simulation framework and tagging methodology. revision: yes

  2. Referee: [Model and benchmarks] Model section: in Type-I 2HDM the light scalar's fermion couplings are scaled by a mixing factor (cos(β-α) or equivalent), which can suppress the partial width to bb relative to gg or ττ; the reach estimates assume BR(h→bb) remains high enough for the signal yield, but no explicit branching-ratio calculations or scans over the mixing angle are shown for the benchmarks.

    Authors: The referee correctly identifies the role of the mixing angle in Type-I 2HDM. For the chosen benchmarks, we selected mixing parameters such that BR(h → bb) remains dominant (approximately 80–90% for mh = 30–70 GeV), consistent with the hierarchical spectrum where the light scalar couplings to fermions are not strongly suppressed. We will add explicit branching-ratio calculations for the benchmarks and a short discussion of the viable mixing-angle range in the revised Model section to make this assumption transparent. revision: yes

  3. Referee: [Analysis and results] Analysis and results: the projected reaches rely on standard Monte Carlo simulations of signal and background without data-driven validation or discussion of how high-pT V + jets backgrounds are controlled after the fat-jet tagging, making the precise luminosity-dependent numbers sensitive to unquantified assumptions.

    Authors: The analysis employs standard Monte Carlo tools for signal and background generation, with high-pT V + jets backgrounds suppressed via the double-b subjet requirement inside the fat-jet together with kinematic cuts on the associated gauge boson. Tagging efficiencies and basic systematic variations are evaluated from simulation. As this is a prospective study for future luminosities, data-driven validation is not feasible; we will expand the Results section with additional discussion of post-tagging background composition and estimated uncertainties on the tagging working point to reduce reliance on unquantified assumptions. revision: partial

Circularity Check

0 steps flagged

No significant circularity in projected exclusion reaches

full rationale

The paper derives projected 2σ exclusion reaches (up to ~540 GeV at HL-LHC) for heavy scalars via Monte Carlo simulation of electroweak production of light h in association with A or H±, followed by boosted h → bb reconstructed as a double-b fat-jet J_bb plus a gauge boson. These reaches are forward projections under stated assumptions on branching ratios, tagging efficiencies, and background control; no parameters are fitted to data subsets inside the paper and then presented as independent predictions. No self-definitional steps, uniqueness theorems imported from the authors' prior work, or ansatze smuggled via self-citation appear in the derivation chain. The analysis relies on standard simulation tools and established jet-tagging methods, making the central claims self-contained against external benchmarks rather than reducing to the paper's own inputs by construction.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claim rests on standard 2HDM model assumptions and collider simulation techniques; no new particles or forces are introduced, and free parameters are limited to benchmark mass choices rather than global fits.

free parameters (1)
  • Light scalar mass benchmarks
    M_h values of 30-70 GeV chosen to illustrate reach for light scalars.
axioms (2)
  • domain assumption Light scalar decays predominantly to b b-bar
    Follows from Type-I 2HDM coupling structure for the chosen parameter space.
  • domain assumption Standard LHC detector response and background modeling
    Used to derive the quoted exclusion limits.

pith-pipeline@v0.9.0 · 5664 in / 1500 out tokens · 84105 ms · 2026-05-14T18:24:29.323786+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

52 extracted references · 47 canonical work pages · 33 internal anchors

  1. [1]

    Phenomenology of a New Minimal Supersymmetric Extension of the Standard Model

    A. Dedes, C. Hugonie, S. Moretti and K. Tamvakis,Phenomenology of a new minimal supersymmetric extension of the standard model,Phys. Rev. D63(2001) 055009 [hep-ph/0009125]

  2. [2]

    B. A. Dobrescu and K. T. Matchev,Light axion within the next-to-minimal supersymmetric standard model,JHEP09(2000) 031 [hep-ph/0008192]

  3. [3]

    Towards a No-Lose Theorem for NMSSM Higgs Discovery at the LHC

    U. Ellwanger, J. F. Gunion, C. Hugonie and S. Moretti,Towards a no lose theorem for NMSSM Higgs discovery at the LHC,hep-ph/0305109

  4. [4]

    Escaping the Large Fine Tuning and Little Hierarchy Problems in the Next to Minimal Supersymmetric Model and h-> aa Decays

    R. Dermisek and J. F. Gunion,Escaping the large fine tuning and little hierarchy problems in the next to minimal supersymmetric model andh→aadecays,Phys. Rev. Lett.95(2005) 041801 [hep-ph/0502105]

  5. [5]

    Secluded WIMP Dark Matter

    M. Pospelov, A. Ritz and M. B. Voloshin,Secluded WIMP Dark Matter,Phys. Lett. B662(2008) 53 [0711.4866]

  6. [6]

    Dark Light Higgs

    P. Draper, T. Liu, C. E. M. Wagner, L.-T. Wang and H. Zhang,Dark Light Higgs,Phys. Rev. Lett. 106(2011) 121805 [1009.3963]

  7. [7]

    S. Ipek, D. McKeen and A. E. Nelson,A Renormalizable Model for the Galactic Center Gamma Ray Excess from Dark Matter Annihilation,Phys. Rev. D90(2014) 055021 [1404.3716]

  8. [8]

    An Updated Analysis of Inert Higgs Doublet Model in light of the Recent Results from LUX, PLANCK, AMS-02 and LHC

    A. Arhrib, Y.-L. S. Tsai, Q. Yuan and T.-C. Yuan,An Updated Analysis of Inert Higgs Doublet Model in light of the Recent Results from LUX, PLANCK, AMS-02 and LHC,JCAP06(2014) 030 [1310.0358]

  9. [9]

    T. D. Lee,A Theory of Spontaneous T Violation,Phys. Rev. D8(1973) 1226

  10. [10]

    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 [1106.0034]. [15]CMScollaboration,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and twoτleptons in proton-proton collisions at √s= 13TeV...

  11. [11]

    Multi-photon production in the Type-I 2HDM

    A. Arhrib, R. Benbrik, S. Moretti, A. Rouchad, Q.-S. Yan and X. Zhang,Multi-photon production in the Type-I 2HDM,JHEP07(2018) 007 [1712.05332]

  12. [12]

    Identifying a light charged Higgs boson at the LHC Run II

    A. Arhrib, R. Benbrik, R. Enberg, W. Klemm, S. Moretti and S. Munir,Identifying a light charged Higgs boson at the LHC Run II,Phys. Lett. B774(2017) 591 [1706.01964]

  13. [13]

    Y. Wang, A. Arhrib, R. Benbrik, M. Krab, B. Manaut, S. Moretti et al.,Analysis of W + 4γin the 2HDM Type-I at the LHC,JHEP12(2021) 021 [2107.01451]

  14. [14]

    J. Kim, S. Lee, P. Sanyal, J. Song and D. Wang,τ ±νγγandℓ ±ℓ±γγ/ET Xto probe the fermiophobic Higgs boson with high cutoff scales,JHEP04(2023) 083 [2302.05467]. [31]CMScollaboration,Search for the exotic decay of the Higgs boson into two light pseudoscalars with four photons in the final state in proton-proton collisions at √s= 13 TeV,JHEP07(2023) 148 [22...

  15. [15]

    J. F. Gunion, H. E. Haber, G. L. Kane and S. Dawson,The Higgs Hunter’s Guide, vol. 80. 2000

  16. [16]

    Basis-independent methods for the two-Higgs-doublet model

    S. Davidson and H. E. Haber,Basis-independent methods for the two-Higgs-doublet model,Phys. Rev. D72(2005) 035004 [hep-ph/0504050]

  17. [17]

    The Anatomy of Electro-Weak Symmetry Breaking. II: The Higgs bosons in the Minimal Supersymmetric Model

    A. Djouadi,The Anatomy of electro-weak symmetry breaking. II. The Higgs bosons in the minimal supersymmetric model,Phys. Rept.459(2008) 1 [hep-ph/0503173]. – 28 –

  18. [18]

    S. L. Glashow and S. Weinberg,Natural Conservation Laws for Neutral Currents,Phys. Rev. D15 (1977) 1958

  19. [19]

    E. A. Paschos,Diagonal Neutral Currents,Phys. Rev. D15(1977) 1966

  20. [20]

    A. G. Akeroyd,Fermiophobic Higgs bosons at the Tevatron,Phys. Lett. B368(1996) 89 [hep-ph/9511347]

  21. [21]

    A. G. Akeroyd,Fermiophobic and other nonminimal neutral Higgs bosons at the LHC,J. Phys. G24 (1998) 1983 [hep-ph/9803324]

  22. [22]

    Bosonic Decays of Charged Higgs Bosons in a 2HDM Type-I

    A. Arhrib, R. Benbrik and S. Moretti,Bosonic Decays of Charged Higgs Bosons in a 2HDM Type-I, Eur. Phys. J. C77(2017) 621 [1607.02402]

  23. [23]

    Electroweak production of multiple (pseudo)scalars in the 2HDM

    R. Enberg, W. Klemm, S. Moretti and S. Munir,Electroweak production of multiple (pseudo)scalars in the 2HDM,Eur. Phys. J. C79(2019) 512 [1812.01147]

  24. [24]

    Kling, S

    F. Kling, S. Su and W. Su,2HDM Neutral Scalars under the LHC,JHEP06(2020) 163 [2004.04172]

  25. [25]

    H. Bahl, T. Stefaniak and J. Wittbrodt,The forgotten channels: charged Higgs boson decays to a W and a non-SM-like Higgs boson,JHEP06(2021) 183 [2103.07484]

  26. [26]

    Arhrib, R

    A. Arhrib, R. Benbrik, M. Krab, B. Manaut, S. Moretti, Y. Wang et al.,New discovery modes for a light charged Higgs boson at the LHC,JHEP10(2021) 073 [2106.13656]

  27. [27]

    Mondal and P

    T. Mondal and P. Sanyal,Same sign trilepton as signature of charged Higgs in two Higgs doublet model,JHEP05(2022) 040 [2109.05682]

  28. [28]

    J. Kim, S. Lee, J. Song and P. Sanyal,Fermiophobic light Higgs boson in the type-I two-Higgs-doublet model,Phys. Lett. B834(2022) 137406 [2207.05104]

  29. [29]

    S. K. Kang, J. Kim, S. Lee and J. Song,Disentangling the high- and low-cutoff scales via the trilinear Higgs couplings in the type-I two-Higgs-doublet model,Phys. Rev. D107(2023) 015025 [2210.00020]

  30. [30]

    Z. Li, A. Arhrib, R. Benbrik, M. Krab, B. Manaut, S. Moretti et al.,Discovering a light charged Higgs boson viaW ±∗ + 4bfinal states at the LHC,2305.05788

  31. [31]

    Mondal, S

    T. Mondal, S. Moretti, S. Munir and P. Sanyal,Electroweak Multi-Higgs Production: A Smoking Gun for the Type-I Two-Higgs-Doublet Model,Phys. Rev. Lett.131(2023) 231801 [2304.07719]

  32. [32]

    Sanyal and D

    P. Sanyal and D. Wang,Probing the electroweak4b+ℓ+/E T final state in type I 2HDM at the LHC, JHEP09(2023) 076 [2305.00659]

  33. [33]

    Arhrib, S

    A. Arhrib, S. Moretti, S. Semlali, C. H. Shepherd-Themistocleous, Y. Wang and Q. S. Yan,Searching for H→hh→bb¯τ τin the 2HDM type-I at the LHC,Phys. Rev. D109(2024) 055020 [2310.02736]

  34. [34]

    E. A. Moreno, T. Q. Nguyen, J.-R. Vlimant, O. Cerri, H. B. Newman, A. Periwal et al.,Interaction networks for the identification of boostedH→b bdecays,Phys. Rev. D102(2020) 012010 [1909.12285]

  35. [35]

    J. Lin, M. Freytsis, I. Moult and B. Nachman,BoostingH→b ¯bwith Machine Learning,JHEP10 (2018) 101 [1807.10768]

  36. [36]

    D. K. Ghosh, B. Mukhopadhyaya, S. Samanta and R. K. Singh,LHC signatures of a light pseudoscalar in a flipped two-Higgs scenario: the usefulness of boostedb ¯bpairs,2604.06937

  37. [37]

    J. F. Gunion and H. E. Haber,The CP conserving two Higgs doublet model: The Approach to the decoupling limit,Phys. Rev. D67(2003) 075019 [hep-ph/0207010]

  38. [38]

    Lee-Quigg-Thacker Bounds for Higgs Boson Masses in a Two-Doublet Model

    S. Kanemura, T. Kubota and E. Takasugi,Lee-Quigg-Thacker bounds for Higgs boson masses in a two doublet model,Phys. Lett. B313(1993) 155 [hep-ph/9303263]

  39. [39]

    A. G. Akeroyd, A. Arhrib and E.-M. Naimi,Note on tree level unitarity in the general two Higgs doublet model,Phys. Lett. B490(2000) 119 [hep-ph/0006035]. – 29 –

  40. [40]

    Tree-unitarity bounds for THDM Higgs masses revisited

    J. Horejsi and M. Kladiva,Tree-unitarity bounds for THDM Higgs masses revisited,Eur. Phys. J. C 46(2006) 81 [hep-ph/0510154]

  41. [41]

    M. E. Peskin and T. Takeuchi,Estimation of oblique electroweak corrections,Phys. Rev. D46(1992) 381

  42. [42]

    2HDMC - Two-Higgs-Doublet Model Calculator

    D. Eriksson, J. Rathsman and O. Stal,2HDMC: Two-Higgs-Doublet Model Calculator Physics and Manual,Comput. Phys. Commun.181(2010) 189 [0902.0851]. [66]Particle Data Groupcollaboration,Review of Particle Physics,PTEP2022(2022) 083C01. [67]HFLA Vcollaboration,Averages ofb-hadron,c-hadron, andτ-lepton properties as of summer 2016, Eur. Phys. J. C77(2017) 895 ...

  43. [43]

    Weak Radiative Decays of the B Meson and Bounds on $M_{H^\pm}$ in the Two-Higgs-Doublet Model

    M. Misiak and M. Steinhauser,Weak radiative decays of the B meson and bounds onM H± in the Two-Higgs-Doublet Model,Eur. Phys. J. C77(2017) 201 [1702.04571]

  44. [44]

    Bechtle, D

    P. Bechtle, D. Dercks, S. Heinemeyer, T. Klingl, T. Stefaniak, G. Weiglein et al.,HiggsBounds-5: Testing Higgs Sectors in the LHC 13 TeV Era,Eur. Phys. J. C80(2020) 1211 [2006.06007]. [70]ALEPH, DELPHI, L3, OPAL, LEP Working Group for Higgs Boson Searchescollaboration, Search for neutral MSSM Higgs bosons at LEP,Eur. Phys. J. C47(2006) 547 [hep-ex/0602042...

  45. [45]

    MadGraph 5 : Going Beyond

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

  46. [46]

    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 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 [1405.0301]

  47. [47]

    FeynRules 2.0 - A complete toolbox for tree-level phenomenology

    A. Alloul, N. D. Christensen, C. Degrande, C. Duhr and B. Fuks,FeynRules 2.0 - A complete toolbox for tree-level phenomenology,Comput. Phys. Commun.185(2014) 2250 [1310.1921]

  48. [48]

    UFO - The Universal FeynRules Output

    C. Degrande, C. Duhr, B. Fuks, D. Grellscheid, O. Mattelaer and T. Reiter,UFO - The Universal FeynRules Output,Comput. Phys. Commun.183(2012) 1201 [1108.2040]

  49. [49]

    PYTHIA 6.4 Physics and Manual

    T. Sjostrand, S. Mrenna and P. Z. Skands,PYTHIA 6.4 Physics and Manual,JHEP05(2006) 026 [hep-ph/0603175]

  50. [50]

    An Introduction to PYTHIA 8.2

    T. Sj ¨ostrand, S. Ask, J. R. Christiansen, R. Corke, N. Desai, P. Ilten et al.,An introduction to PYTHIA 8.2,Comput. Phys. Commun.191(2015) 159 [1410.3012]. [79]DELPHES 3collaboration,DELPHES 3, A modular framework for fast simulation of a generic collider experiment,JHEP02(2014) 057 [1307.6346]

  51. [51]

    FastJet user manual

    M. Cacciari, G. P. Salam and G. Soyez,FastJet User Manual,Eur. Phys. J. C72(2012) 1896 [1111.6097]

  52. [52]

    The anti-k_t jet clustering algorithm

    M. Cacciari, G. P. Salam and G. Soyez,The anti-k t jet clustering algorithm,JHEP04(2008) 063 [0802.1189]. [82]CMScollaboration,Measurement of boosted Higgs bosons produced via vector boson fusion or gluon fusion in the H→b b decay mode using LHC proton-proton collision data at √s= 13 TeV,JHEP12 (2024) 035 [2407.08012]. – 30 –