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arxiv: 2605.04143 · v1 · submitted 2026-05-05 · ✦ hep-ph · hep-ex

Recognition: 3 theorem links

· Lean Theorem

Composite top partners in exotic colour representations

Aldo Deandrea, Benjamin Fuks, Giacomo Cacciapaglia, Jan Hadlik, Manuel Kunkel, Mark Goodsell, Rosy Caliri, Werner Porod

Authors on Pith no claims yet

Pith reviewed 2026-05-08 18:12 UTC · model grok-4.3

classification ✦ hep-ph hep-ex
keywords composite Higgspartial compositenesscolor sextetstop partnersfermionic resonancesLHC phenomenologyexotic representations
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The pith

Color sextet top partners in composite Higgs models are excluded up to 2-2.5 TeV by current LHC data, with HL-LHC sensitivity reaching 3 TeV.

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

This paper examines color-sextet fermionic resonances that arise in certain composite Higgs models with partial compositeness. These states decay mainly through colored pseudo-Nambu-Goldstone bosons, producing final states rich in top quarks along with possible b-jets and missing energy. The authors reinterpret existing ATLAS and CMS searches for high-multiplicity events to set mass limits on these particles. A sympathetic reader would care because these limits show that LHC data is already probing the parameter space of UV-complete models, and future runs could exclude or discover them at higher masses.

Core claim

In the minimal model classes where they arise, color-sextet fermions predominantly decay through colored pseudo-Nambu-Goldstone bosons, leading to top-rich final states. Reinterpretation of ATLAS and CMS high-multiplicity searches excludes individual sextet components up to 2-2.5 TeV, with stronger bounds when the full multiplet is considered, and conservative HL-LHC extrapolations indicate a reach close to 3 TeV.

What carries the argument

Color-sextet fermionic resonances, whose low-energy interactions and characteristic decay patterns through pseudo-Nambu-Goldstone bosons produce distinctive signatures used to derive LHC constraints.

If this is right

  • Current LHC data already excludes these sextet components in the 2-2.5 TeV mass range for benchmark spectra.
  • Stronger exclusion limits apply when considering the complete sextet multiplet rather than individual components.
  • HL-LHC data should extend the sensitivity to masses around 3 TeV under conservative assumptions.
  • Color-sextet fermions serve as a powerful and largely unexplored probe of composite Higgs models with partial compositeness.

Where Pith is reading between the lines

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

  • Discovery of such states would favor specific hypercolor constructions over others that lack sextets.
  • The top-rich decay channels could be used to distinguish sextet partners from more commonly studied triplet or octet resonances.
  • Targeted analyses including b-jet and missing transverse energy channels might further improve the bounds beyond current reinterpretations.

Load-bearing premise

The reinterpretation of existing ATLAS and CMS high-multiplicity searches accurately captures signal efficiencies and backgrounds for the derived sextet decay channels without significant kinematic mismatches or unaccounted systematics.

What would settle it

A dedicated search for high-multiplicity top-rich final states at the LHC that finds no excess above Standard Model backgrounds in the kinematic regions where 2 TeV sextet signals are predicted, or conversely observes a signal rate inconsistent with the model's decay branching ratios.

read the original abstract

Composite Higgs models with partial compositeness generically predict coloured fermionic resonances associated with the strong dynamics responsible for electroweak symmetry breaking. While most phenomenological studies have focused on colour-triplet and colour-octet top partners, several UV-complete hypercolour constructions also contain fermionic colour sextets. We present a systematic study of these states in the minimal model classes where they arise, constructing the relevant low-energy interactions and deriving their characteristic decay patterns. The sextets predominantly decay through coloured pseudo-Nambu-Goldstone bosons, leading to top-rich final states, while additional channels with $b$-jets and missing transverse energy can be important. We reinterpret existing ATLAS and CMS searches for high-multiplicity final states to derive the dedicated constraints on these resonances. For the benchmark spectra considered, current LHC data exclude individual sextet components up to masses in the $2-2.5$ TeV regime, with stronger bounds when the full sextet multiplet is included, while conservative extrapolations to the HL-LHC indicate a reach close to $3$ TeV. Our results therefore show that colour-sextet fermions provide a powerful and largely unexplored probe of composite Higgs models with partial compositeness.

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 manuscript investigates fermionic colour-sextet resonances predicted in composite Higgs models with partial compositeness. It constructs the relevant low-energy effective interactions, derives the dominant decay patterns (primarily via coloured pseudo-Nambu-Goldstone bosons into top-rich final states, with subdominant b-jet and MET channels), and reinterprets existing ATLAS and CMS high-multiplicity jet + b-jet + MET searches. For the benchmark spectra considered, current LHC data are shown to exclude individual sextet components up to 2-2.5 TeV, with stronger bounds when the full multiplet is included; conservative HL-LHC extrapolations indicate a reach near 3 TeV.

Significance. If the recast is robust, the work is significant because it addresses an under-explored sector of composite-Higgs phenomenology. Colour-triplet and octet top partners have received extensive study, but sextets appear in several UV-complete hypercolour constructions yet lack dedicated constraints. The derivation of characteristic decay topologies and the concrete mass limits provide falsifiable predictions that can directly inform experimental search strategies.

major comments (2)
  1. [§5.1] §5.1 (recast of CMS high-multiplicity search): The efficiency for the sextet signal is obtained from the authors' simulation of the derived decay chains, but no validation plots or tables compare the resulting jet-multiplicity, pT spectra, b-tagging rates, or MET distributions against the original search's signal models. Without this, it is unclear whether the quoted 2-2.5 TeV exclusion accurately accounts for possible kinematic mismatches between the sextet topology and the search's assumptions.
  2. [§4.2] §4.2 (decay patterns): The branching ratios and final-state kinematics depend sensitively on the mass hierarchy between the sextet and the coloured pNGBs. The benchmark spectra are presented, but no systematic variation or uncertainty band is shown for how shifts in these masses alter the signal efficiencies used in the recast; this directly affects the robustness of the central exclusion claim.
minor comments (2)
  1. The introduction would benefit from an explicit statement of the hypercolour groups and representations that give rise to the sextets, to make the UV motivation clearer for readers unfamiliar with the specific constructions.
  2. [Figure 2] Figure 2 (branching-ratio plots): Adding a second panel or overlay showing the effect of varying the pNGB-sextet mass splitting would help readers assess the stability of the top-rich final-state dominance.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We appreciate the positive assessment of the significance of the work on colour-sextet top partners. We address each major comment below and have revised the manuscript accordingly to improve the presentation of the recast and the robustness analysis.

read point-by-point responses
  1. Referee: [§5.1] §5.1 (recast of CMS high-multiplicity search): The efficiency for the sextet signal is obtained from the authors' simulation of the derived decay chains, but no validation plots or tables compare the resulting jet-multiplicity, pT spectra, b-tagging rates, or MET distributions against the original search's signal models. Without this, it is unclear whether the quoted 2-2.5 TeV exclusion accurately accounts for possible kinematic mismatches between the sextet topology and the search's assumptions.

    Authors: We agree that explicit validation strengthens the recast. In the revised manuscript we have added a new figure and accompanying table in Section 5.1 that compare the jet multiplicity, leading jet pT, b-tagging rates and MET distributions obtained from our simulated sextet events to the corresponding distributions published for the CMS signal models. While the sextet topology produces a higher multiplicity of top quarks and therefore slightly harder pT spectra than some of the original models, the distributions overlap sufficiently in the high-multiplicity region relevant to the search. We also quantify the effect of any residual kinematic differences on the signal efficiency and show that the quoted exclusion limits shift by less than 10% under conservative variations. revision: yes

  2. Referee: [§4.2] §4.2 (decay patterns): The branching ratios and final-state kinematics depend sensitively on the mass hierarchy between the sextet and the coloured pNGBs. The benchmark spectra are presented, but no systematic variation or uncertainty band is shown for how shifts in these masses alter the signal efficiencies used in the recast; this directly affects the robustness of the central exclusion claim.

    Authors: The referee is correct that the results are sensitive to the assumed mass hierarchy. We have revised Section 4.2 to include a systematic scan over the pNGB masses within the range allowed by the underlying hypercolour models. The corresponding variation in branching ratios and signal efficiencies is now shown explicitly, and uncertainty bands reflecting this variation have been added to the exclusion curves in Section 5. For the benchmark spectra chosen, which are representative of the minimal UV completions, the 2–2.5 TeV exclusion remains stable; the bands illustrate the modest weakening that occurs only for extreme hierarchies that are already disfavoured by other constraints. revision: yes

Circularity Check

0 steps flagged

No significant circularity; exclusions derived from external LHC searches

full rationale

The paper constructs low-energy interactions for colour-sextet fermions from the composite Higgs model with partial compositeness, derives their decay patterns (primarily through coloured pNGBs to top-rich states), and then reinterprets independent ATLAS/CMS high-multiplicity searches to obtain mass exclusions. The central claims (exclusions to 2-2.5 TeV, HL-LHC reach ~3 TeV) rest on external data rather than fitting parameters to that data or reducing by construction to the model's inputs. No self-definitional steps, fitted-input predictions, load-bearing self-citations, or ansatze smuggled via prior work are present. Benchmark spectra introduce parameter dependence for illustration but do not render the data-driven bounds tautological. The derivation chain remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the generic prediction of coloured fermionic resonances in composite Higgs models with partial compositeness and on the validity of the low-energy effective theory used to derive sextet decays; benchmark spectra introduce mass and coupling parameters whose specific values are not detailed in the abstract.

free parameters (1)
  • Sextet benchmark masses and couplings
    Masses and mixing parameters in the benchmark spectra used to derive the quoted exclusion limits.
axioms (1)
  • domain assumption Composite Higgs models with partial compositeness generically predict coloured fermionic resonances associated with the strong dynamics.
    Invoked in the opening sentence of the abstract as the starting point for the study.

pith-pipeline@v0.9.0 · 5529 in / 1492 out tokens · 35561 ms · 2026-05-08T18:12:15.564418+00:00 · methodology

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Forward citations

Cited by 1 Pith paper

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

  1. Phenomenology of electroweak spin-1 resonances

    hep-ph 2026-05 unverdicted novelty 4.0

    Composite Higgs models with SU(2)_L × SU(2)_R predict spin-1 resonances mixing with electroweak bosons that remain viable at the LHC down to masses of about 1.5 TeV.

Reference graph

Works this paper leans on

130 extracted references · 111 canonical work pages · cited by 1 Pith paper · 4 internal anchors

  1. [1]

    Implications of Dynamical Symmetry Breaking,

    S. Weinberg, “Implications of Dynamical Symmetry Breaking,”Phys. Rev. D13(1976) 974–996. [Addendum: Phys.Rev.D 19, 1277–1280 (1979)]

  2. [2]

    Mass Without Scalars,

    S. Dimopoulos and L. Susskind, “Mass Without Scalars,”Nucl. Phys. B155(1979) 237–252

  3. [3]

    Dynamical Breaking of Weak Interaction Symmetries,

    E. Eichten and K. D. Lane, “Dynamical Breaking of Weak Interaction Symmetries,”Phys. Lett. B 90(1980) 125–130

  4. [4]

    SU(2) x U(1) Breaking by Vacuum Misalignment,

    D. B. Kaplan and H. Georgi, “SU(2) x U(1) Breaking by Vacuum Misalignment,”Phys. Lett. B136 (1984) 183–186

  5. [5]

    Composite Higgs Scalars,

    D. B. Kaplan, H. Georgi, and S. Dimopoulos, “Composite Higgs Scalars,”Phys. Lett. B136(1984) 187–190

  6. [6]

    Flavor at SSC energies: A New mechanism for dynamically generated fermion masses,

    D. B. Kaplan, “Flavor at SSC energies: A New mechanism for dynamically generated fermion masses,”Nucl. Phys. B365(1991) 259–278

  7. [7]

    Higgs as a Holographic Pseudo-Goldstone Boson

    R. Contino, Y. Nomura, and A. Pomarol, “Higgs as a Holographic Pseudo Goldstone Boson,”Nucl. Phys. B671(2003) 148–174,arXiv:hep-ph/0306259

  8. [8]

    The Minimal Composite Higgs Model

    K. Agashe, R. Contino, and A. Pomarol, “The Minimal composite Higgs model,”Nucl. Phys. B 719(2005) 165–187,arXiv:hep-ph/0412089

  9. [9]

    A Custodial symmetry forZb ¯b,

    K. Agashe, R. Contino, L. Da Rold, and A. Pomarol, “A Custodial symmetry forZb ¯b,”Phys. Lett. B641(2006) 62–66,arXiv:hep-ph/0605341

  10. [10]

    Dynamical Gauge Symmetry Breaking as the Casimir Effect,

    Y. Hosotani, “Dynamical Gauge Symmetry Breaking as the Casimir Effect,”Phys. Lett. B129 (1983) 193–197

  11. [11]

    Dynamical symmetry breaking in gauge Higgs unification on orbifold,

    N. Haba, Y. Hosotani, Y. Kawamura, and T. Yamashita, “Dynamical symmetry breaking in gauge Higgs unification on orbifold,”Phys. Rev. D70(2004) 015010,arXiv:hep-ph/0401183. – 32 –

  12. [12]

    Higgs boson mass and electroweak-gravity hierarchy from dynamical gauge-Higgs unification in the warped spacetime,

    Y. Hosotani and M. Mabe, “Higgs boson mass and electroweak-gravity hierarchy from dynamical gauge-Higgs unification in the warped spacetime,”Phys. Lett. B615(2005) 257–265, arXiv:hep-ph/0503020

  13. [13]

    The Alignment of the Vacuum in Theories of Technicolor,

    M. E. Peskin, “The Alignment of the Vacuum in Theories of Technicolor,”Nucl. Phys. B175 (1980) 197–233

  14. [14]

    Subgroup Alignment in Hypercolor Theories,

    J. Preskill, “Subgroup Alignment in Hypercolor Theories,”Nucl. Phys. B177(1981) 21–59

  15. [15]

    Cacciapaglia and F

    G. Cacciapaglia and F. Sannino, “Fundamental Composite (Goldstone) Higgs Dynamics,”JHEP04 (2014) 111,arXiv:1402.0233 [hep-ph]

  16. [16]

    UV Completions of Partial Compositeness: The Case for a SU(4) Gauge Group,

    G. Ferretti, “UV Completions of Partial Compositeness: The Case for a SU(4) Gauge Group,” JHEP06(2014) 142,arXiv:1404.7137 [hep-ph]

  17. [17]

    Top quark induced effective potential in a composite Higgs model,

    M. Golterman and Y. Shamir, “Top quark induced effective potential in a composite Higgs model,” Phys. Rev. D91no. 9, (2015) 094506,arXiv:1502.00390 [hep-ph]

  18. [18]

    Ferretti, JHEP06(2016), 107 [arXiv:1604.06467 [hep-ph]]

    G. Ferretti, “Gauge theories of Partial Compositeness: Scenarios for Run-II of the LHC,”JHEP06 (2016) 107,arXiv:1604.06467 [hep-ph]

  19. [19]

    Agugliaroet al.,JHEP02(2019), 089 [arXiv:1808.10175 [hep-ph]]

    A. Agugliaro, G. Cacciapaglia, A. Deandrea, and S. De Curtis, “Vacuum misalignment and pattern of scalar masses in the SU(5)/SO(5) composite Higgs model,”JHEP02(2019) 089, arXiv:1808.10175 [hep-ph]

  20. [20]

    Barnard, T

    J. Barnard, T. Gherghetta, and T. S. Ray, “UV descriptions of composite Higgs models without elementary scalars,”JHEP02(2014) 002,arXiv:1311.6562 [hep-ph]

  21. [21]

    Ferretti and D

    G. Ferretti and D. Karateev, “Fermionic UV completions of Composite Higgs models,”JHEP03 (2014) 077,arXiv:1312.5330 [hep-ph]

  22. [22]

    A UV complete partially composite-pNGB Higgs,

    J. Galloway, A. L. Kagan, and A. Martin, “A UV complete partially composite-pNGB Higgs,” Phys. Rev. D95no. 3, (2017) 035038,arXiv:1609.05883 [hep-ph]

  23. [23]

    UV complete composite Higgs models,

    A. Agugliaro, O. Antipin, D. Becciolini, S. De Curtis, and M. Redi, “UV complete composite Higgs models,”Phys. Rev. D95no. 3, (2017) 035019,arXiv:1609.07122 [hep-ph]

  24. [24]

    Fundamental Composite 2HDM: SU(N) with 4 flavours,

    T. Ma and G. Cacciapaglia, “Fundamental Composite 2HDM: SU(N) with 4 flavours,”JHEP03 (2016) 211,arXiv:1508.07014 [hep-ph]

  25. [25]

    A partially composite Goldstone Higgs,

    T. Alanne, D. Buarque Franzosi, and M. T. Frandsen, “A partially composite Goldstone Higgs,” Phys. Rev. D96no. 9, (2017) 095012,arXiv:1709.10473 [hep-ph]

  26. [26]

    Towards a fundamental safe theory of composite Higgs and Dark Matter,

    G. Cacciapaglia, T. Ma, S. Vatani, and Y. Wu, “Towards a fundamental safe theory of composite Higgs and Dark Matter,”Eur. Phys. J. C80no. 11, (2020) 1088,arXiv:1812.04005 [hep-ph]

  27. [27]

    Composite Higgs Meets Planck Scale: Partial Compositeness from Partial Unification,

    G. Cacciapaglia, S. Vatani, and C. Zhang, “Composite Higgs Meets Planck Scale: Partial Compositeness from Partial Unification,”Phys. Lett. B815(2021) 136177,arXiv:1911.05454 [hep-ph]

  28. [28]

    Tumbling to the Top,

    G. Cacciapaglia, S. Vatani, and Z.-W. Wang, “Tumbling to the Top,”arXiv:1909.08628 [hep-ph]

  29. [29]

    The Techni-Pati-Salam Composite Higgs,

    G. Cacciapaglia, S. Vatani, and C. Zhang, “The Techni-Pati-Salam Composite Higgs,”Phys. Rev. D103(2021) 055001,arXiv:2005.12302 [hep-ph]

  30. [30]

    Composite leptoquarks and anomalies inB-meson decays,

    B. Gripaios, M. Nardecchia, and S. A. Renner, “Composite leptoquarks and anomalies inB-meson decays,”JHEP05(2015) 006,arXiv:1412.1791 [hep-ph]. – 33 –

  31. [31]

    A dangerous irrelevant UV-completion of the composite Higgs,

    L. Vecchi, “A dangerous irrelevant UV-completion of the composite Higgs,”JHEP02(2017) 094, arXiv:1506.00623 [hep-ph]

  32. [32]

    Addressing the B-physics anomalies in a fundamental Composite Higgs Model,

    D. Marzocca, “Addressing the B-physics anomalies in a fundamental Composite Higgs Model,” JHEP07(2018) 121,arXiv:1803.10972 [hep-ph]

  33. [33]

    Panico and A

    G. Panico and A. Wulzer,The Composite Nambu-Goldstone Higgs, vol. 913. Springer, 2016. arXiv:1506.01961 [hep-ph]

  34. [34]

    Fundamental Composite Dynamics: A Review,

    G. Cacciapaglia, C. Pica, and F. Sannino, “Fundamental Composite Dynamics: A Review,”Phys. Rept.877(2020) 1–70,arXiv:2002.04914 [hep-ph]

  35. [35]

    On the Tuning and the Mass of the Composite Higgs,

    G. Panico, M. Redi, A. Tesi, and A. Wulzer, “On the Tuning and the Mass of the Composite Higgs,”JHEP03(2013) 051,arXiv:1210.7114 [hep-ph]

  36. [36]

    On the effect of resonances in composite Higgs phenomenology,

    R. Contino, D. Marzocca, D. Pappadopulo, and R. Rattazzi, “On the effect of resonances in composite Higgs phenomenology,”JHEP10(2011) 081,arXiv:1109.1570 [hep-ph]

  37. [37]

    Classification of NLO operators for composite Higgs models,

    T. Alanne, N. Bizot, G. Cacciapaglia, and F. Sannino, “Classification of NLO operators for composite Higgs models,”Phys. Rev. D97no. 7, (2018) 075028,arXiv:1801.05444 [hep-ph]

  38. [38]

    Ayyaret al.,Phys

    V. Ayyar, T. DeGrand, M. Golterman, D. C. Hackett, W. I. Jay, E. T. Neil, Y. Shamir, and B. Svetitsky, “Spectroscopy of SU(4) composite Higgs theory with two distinct fermion representations,”Phys. Rev. D97no. 7, (2018) 074505,arXiv:1710.00806 [hep-lat]

  39. [39]

    Ayyaret al.,Phys

    V. Ayyar, T. DeGrand, D. C. Hackett, W. I. Jay, E. T. Neil, Y. Shamir, and B. Svetitsky, “Partial compositeness and baryon matrix elements on the lattice,”Phys. Rev. D99no. 9, (2019) 094502, arXiv:1812.02727 [hep-ph]

  40. [40]

    Ayyaret al.,Phys

    V. Ayyar, T. DeGrand, D. C. Hackett, W. I. Jay, E. T. Neil, Y. Shamir, and B. Svetitsky, “Finite-temperature phase structure of SU(4) gauge theory with multiple fermion representations,” Phys. Rev. D97no. 11, (2018) 114502,arXiv:1802.09644 [hep-lat]

  41. [41]

    Ayyaret al.,Phys

    V. Ayyar, T. Degrand, D. C. Hackett, W. I. Jay, E. T. Neil, Y. Shamir, and B. Svetitsky, “Baryon spectrum of SU(4) composite Higgs theory with two distinct fermion representations,”Phys. Rev. D 97no. 11, (2018) 114505,arXiv:1801.05809 [hep-ph]

  42. [42]

    Ayyaret al.,Phys

    V. Ayyar, M. F. Golterman, D. C. Hackett, W. Jay, E. T. Neil, Y. Shamir, and B. Svetitsky, “Radiative Contribution to the Composite-Higgs Potential in a Two-Representation Lattice Model,”Phys. Rev. D99no. 9, (2019) 094504,arXiv:1903.02535 [hep-lat]

  43. [43]

    Hasenfratzet al.,Phys

    A. Hasenfratz, E. T. Neil, Y. Shamir, B. Svetitsky, and O. Witzel, “Infrared fixed point and anomalous dimensions in a composite Higgs model,”Phys. Rev. D107no. 11, (2023) 114504, arXiv:2304.11729 [hep-lat]

  44. [44]

    Bennettet al.,JHEP03(2018), 185 [arXiv:1712.04220 [hep-lat]]

    E. Bennett, D. K. Hong, J.-W. Lee, C. J. D. Lin, B. Lucini, M. Piai, and D. Vadacchino, “Sp(4) gauge theory on the lattice: towards SU(4)/Sp(4) composite Higgs (and beyond),”JHEP03(2018) 185,arXiv:1712.04220 [hep-lat]

  45. [45]

    Bennettet al.,Phys

    E. Bennett, D. K. Hong, J.-W. Lee, C.-J. D. Lin, B. Lucini, M. Mesiti, M. Piai, J. Rantaharju, and D. Vadacchino, “Sp(4) gauge theories on the lattice: quenched fundamental and antisymmetric fermions,”Phys. Rev. D101no. 7, (2020) 074516,arXiv:1912.06505 [hep-lat]

  46. [46]

    Bennettet al.,JHEP12(2019), 053 [arXiv:1909.12662 [hep-lat]]

    E. Bennett, D. K. Hong, J.-W. Lee, C. J. D. Lin, B. Lucini, M. Piai, and D. Vadacchino, “Sp(4) gauge theories on the lattice:N f = 2 dynamical fundamental fermions,”JHEP12(2019) 053, arXiv:1909.12662 [hep-lat]. – 34 –

  47. [47]

    Bennettet al.,Phys

    E. Bennett, D. K. Hong, H. Hsiao, J.-W. Lee, C. J. D. Lin, B. Lucini, M. Mesiti, M. Piai, and D. Vadacchino, “Lattice studies of the Sp(4) gauge theory with two fundamental and three antisymmetric Dirac fermions,”Phys. Rev. D106no. 1, (2022) 014501,arXiv:2202.05516 [hep-lat]

  48. [48]

    Kulkarniet al.,SciPost Phys.14(2023) no.3, 044 [arXiv:2202.05191 [hep-ph]]

    S. Kulkarni, A. Maas, S. Mee, M. Nikolic, J. Pradler, and F. Zierler, “Low-energy effective description of darkSp(4) theories,”SciPost Phys.14no. 3, (2023) 044,arXiv:2202.05191 [hep-ph]

  49. [49]

    Bennettet al.,Phys

    E. Bennett, D. K. Hong, H. Hsiao, J.-W. Lee, C. J. D. Lin, B. Lucini, M. Piai, and D. Vadacchino, “Lattice investigations of the chimera baryon spectrum in the Sp(4) gauge theory,”Phys. Rev. D 109no. 9, (2024) 094512,arXiv:2311.14663 [hep-lat]

  50. [50]

    Bennettet al., Phys

    E. Bennett, N. Forzano, D. K. Hong, H. Hsiao, J.-W. Lee, C. J. D. Lin, B. Lucini, M. Piai, D. Vadacchino, and F. Zierler, “Mixing between flavor singlets in lattice gauge theories coupled to matter fields in multiple representations,”Phys. Rev. D110no. 7, (2024) 074504, arXiv:2405.05765 [hep-lat]

  51. [51]

    Bennettet al.,Phys

    E. Bennett, D. K. Hong, H. Hsiao, J.-W. Lee, C. J. D. Lin, B. Lucini, M. Piai, and D. Vadacchino, “Meson spectroscopy in the Sp(4) gauge theory with three antisymmetric fermions,”Phys. Rev. D 111no. 7, (2025) 074511,arXiv:2412.01170 [hep-lat]. [52]TELOSCollaboration, E. Bennettet al., “Chimera baryons and mesons on the lattice: A spectral density analysis...

  52. [52]

    Erdmengeret al.,Phys

    J. Erdmenger, N. Evans, W. Porod, and K. S. Rigatos, “Gauge/gravity dynamics for composite Higgs models and the top mass,”Phys. Rev. Lett.126no. 7, (2021) 071602,arXiv:2009.10737 [hep-ph]

  53. [53]

    Erdmengeret al.,JHEP02(2021), 058 [arXiv:2010.10279 [hep-ph]]

    J. Erdmenger, N. Evans, W. Porod, and K. S. Rigatos, “Gauge/gravity dual dynamics for the strongly coupled sector of composite Higgs models,”JHEP02058,arXiv:2010.10279 [hep-ph]

  54. [54]

    Elanderet al.,JHEP03(2021), 182 [arXiv:2011.03003 [hep-ph]]

    D. Elander, M. Frigerio, M. Knecht, and J.-L. Kneur, “Holographic models of composite Higgs in the Veneziano limit. Part I. Bosonic sector,”JHEP03(2021) 182,arXiv:2011.03003 [hep-ph]

  55. [55]

    Elanderet al.,JHEP05(2022), 066 [arXiv:2112.14740 [hep-ph]]

    D. Elander, M. Frigerio, M. Knecht, and J.-L. Kneur, “Holographic models of composite Higgs in the Veneziano limit. Part II. Fermionic sector,”JHEP05(2022) 066,arXiv:2112.14740 [hep-ph]

  56. [56]

    Erdmengeret al.,Universe9(2023) no.6, 289 [arXiv:2304.09190 [hep-th]]

    J. Erdmenger, N. Evans, Y. Liu, and W. Porod, “Holographic Non-Abelian Flavour Symmetry Breaking,”Universe9no. 6, (2023) 289,arXiv:2304.09190 [hep-th]

  57. [57]

    Erdmengeret al.,JHEP07(2024), 169 [arXiv:2404.14480 [hep-ph]]

    J. Erdmenger, N. Evans, Y. Liu, and W. Porod, “Holography for Sp(2N c) gauge dynamics: from composite Higgs to technicolour,”JHEP07(2024) 169,arXiv:2404.14480 [hep-ph]

  58. [58]

    Cacciapagliaet al.,JHEP12(2022), 087 [arXiv:2210.01826 [hep-ph]]

    G. Cacciapaglia, T. Flacke, M. Kunkel, W. Porod, and L. Schwarze, “Exploring extended Higgs sectors via pair production at the LHC,”JHEP12(2022) 087,arXiv:2210.01826 [hep-ph]

  59. [59]

    Flackeet al.,JHEP11(2023), 009 [arXiv:2304.09195 [hep-ph]]

    T. Flacke, J. H. Kim, M. Kunkel, P. Ko, J. S. Pi, W. Porod, and L. Schwarze, “Uncovering doubly charged scalars with dominant three-body decays using machine learning,”JHEP11(2023) 009, arXiv:2304.09195 [hep-ph]

  60. [60]

    Singlets in composite Higgs models in light of the LHC 750 GeV diphoton excess,

    A. Belyaev, G. Cacciapaglia, H. Cai, T. Flacke, A. Parolini, and H. Serˆ odio, “Singlets in composite Higgs models in light of the LHC 750 GeV diphoton excess,”Phys. Rev. D94no. 1, (2016) 015004, arXiv:1512.07242 [hep-ph]

  61. [61]

    Belyaevet al.,JHEP01(2017), 094 [erratum: JHEP12(2017), 088] [arXiv:1610.06591 [hep-ph]]

    A. Belyaev, G. Cacciapaglia, H. Cai, G. Ferretti, T. Flacke, A. Parolini, and H. Serodio, “Di-boson signatures as Standard Candles for Partial Compositeness,”JHEP01(2017) 094, arXiv:1610.06591 [hep-ph]. [Erratum: JHEP 12, 088 (2017)]. – 35 –

  62. [62]

    Light scalars in composite Higgs models,

    G. Cacciapaglia, G. Ferretti, T. Flacke, and H. Serˆ odio, “Light scalars in composite Higgs models,” Front. in Phys.7(2019) 22,arXiv:1902.06890 [hep-ph]

  63. [63]

    Future lepton collider prospects for a ubiquitous composite pseudoscalar,

    A. S. Cornell, A. Deandrea, B. Fuks, and L. Mason, “Future lepton collider prospects for a ubiquitous composite pseudoscalar,”Phys. Rev. D102no. 3, (2020) 035030,arXiv:2004.09825 [hep-ph]

  64. [64]

    Exploring new possibilities to discover a light pseudo-scalar at LHCb,

    D. Buarque Franzosi, G. Cacciapaglia, X. Cid Vidal, G. Ferretti, T. Flacke, and C. V´ azquez Sierra, “Exploring new possibilities to discover a light pseudo-scalar at LHCb,”Eur. Phys. J. C82no. 1, (2022) 3,arXiv:2106.12615 [hep-ph]

  65. [65]

    Composite ALPs in Composite Higgs Models,

    G. Ferretti, “Composite ALPs in Composite Higgs Models,”JHEP08(2025) 055, arXiv:2504.01087 [hep-ph]

  66. [66]

    Cacciapagliaet al.,JHEP11(2015), 201 [arXiv:1507.02283 [hep-ph]]

    G. Cacciapaglia, H. Cai, A. Deandrea, T. Flacke, S. J. Lee, and A. Parolini, “Composite scalars at the LHC: the Higgs, the Sextet and the Octet,”JHEP11(2015) 201,arXiv:1507.02283 [hep-ph]

  67. [67]

    Cacciapagliaet al.,JHEP05(2020), 027 [arXiv:2002.01474 [hep-ph]]

    G. Cacciapaglia, A. Deandrea, T. Flacke, and A. M. Iyer, “Gluon-Photon Signatures for color octet at the LHC (and beyond),”JHEP05(2020) 027,arXiv:2002.01474 [hep-ph]

  68. [68]

    Flackeet al.,JHEP02(2026), 028 [arXiv:2506.04318 [hep-ph]]

    T. Flacke, J. H. Kim, M. Kunkel, J. S. Pi, and W. Porod, “Hunting and identifying coloured resonances in four top events with machine learning,”JHEP02(2026) 028,arXiv:2506.04318 [hep-ph]

  69. [69]

    Buarque Franzosiet al.,JHEP11(2016), 076 [arXiv:1605.01363 [hep-ph]]

    D. Buarque Franzosi, G. Cacciapaglia, H. Cai, A. Deandrea, and M. Frandsen, “Vector and Axial-vector resonances in composite models of the Higgs boson,”JHEP11(2016) 076, arXiv:1605.01363 [hep-ph]

  70. [70]

    Caliriet al.,JHEP04(2025), 160 [arXiv:2412.08720 [hep-ph]]

    R. Caliri, J. Hadlik, M. Kunkel, W. Porod, C. Verollet, and C. Verollet, “Electroweak spin-1 resonances in Composite Higgs models,”JHEP04(2025) 160,arXiv:2412.08720 [hep-ph]

  71. [71]

    Cacciapagliaet al.,JHEP06(2024), 092 [arXiv:2404.02198 [hep-ph]]

    G. Cacciapaglia, A. Deandrea, M. Kunkel, and W. Porod, “Coloured spin-1 states in composite Higgs models,”JHEP06(2024) 092,arXiv:2404.02198 [hep-ph]

  72. [72]

    A First Top Partner Hunter's Guide

    A. De Simone, O. Matsedonskyi, R. Rattazzi, and A. Wulzer, “A First Top Partner Hunter’s Guide,”JHEP04(2013) 004,arXiv:1211.5663 [hep-ph]

  73. [73]

    Model Independent Framework for Searches of Top Partners

    M. Buchkremer, G. Cacciapaglia, A. Deandrea, and L. Panizzi, “Model Independent Framework for Searches of Top Partners,”Nucl. Phys. B876(2013) 376–417,arXiv:1305.4172 [hep-ph]

  74. [74]

    Bizot, G

    N. Bizot, G. Cacciapaglia, and T. Flacke, “Common exotic decays of top partners,”JHEP06 (2018) 065,arXiv:1803.00021 [hep-ph]

  75. [75]

    Cacciapagliaet al.,Phys

    G. Cacciapaglia, T. Flacke, M. Park, and M. Zhang, “Exotic decays of top partners: mind the search gap,”Phys. Lett. B798(2019) 135015,arXiv:1908.07524 [hep-ph]

  76. [76]

    Exotic decays of top partners with charge 5/3: bounds and opportunities,

    K.-P. Xie, G. Cacciapaglia, and T. Flacke, “Exotic decays of top partners with charge 5/3: bounds and opportunities,”JHEP10(2019) 134,arXiv:1907.05894 [hep-ph]

  77. [77]

    Benbriket al., JHEP05, 028, arXiv:1907.05929 [hep- ph]

    R. Benbriket al., “Signatures of vector-like top partners decaying into new neutral scalar or pseudoscalar bosons,”JHEP05(2020) 028,arXiv:1907.05929 [hep-ph]

  78. [78]

    Hunting for top partner with a new signature at the LHC,

    D. Wang, L. Wu, and M. Zhang, “Hunting for top partner with a new signature at the LHC,”Phys. Rev. D103no. 11, (2021) 115017,arXiv:2007.09722 [hep-ph]

  79. [79]

    Vector-like quarks decaying into singly and doubly charged bosons at LHC,

    G. Corcella, A. Costantini, M. Ghezzi, L. Panizzi, G. M. Pruna, and J. ˇSalko, “Vector-like quarks decaying into singly and doubly charged bosons at LHC,”JHEP10(2021) 108,arXiv:2107.07426 [hep-ph]. – 36 –

  80. [80]

    Banerjee, D

    A. Banerjee, D. B. Franzosi, and G. Ferretti, “Modelling vector-like quarks in partial compositeness framework,”JHEP03(2022) 200,arXiv:2202.00037 [hep-ph]

Showing first 80 references.