pith. sign in

arxiv: 2606.30760 · v1 · pith:ORC7NU3Bnew · submitted 2026-06-29 · ✦ hep-ph · hep-ex

Rich Phenomenology from Simple Ingredients: A Review of Confining Dark Sectors

Pith reviewed 2026-07-01 01:50 UTC · model grok-4.3

classification ✦ hep-ph hep-ex
keywords confining dark sectorscomposite dark matternon-Abelian gauge theoriesdark mesonsdark baryonsabundance similaritydark matter phenomenologycosmology
0
0 comments X

The pith

Confining dark sectors built from new non-Abelian gauge forces produce composite dark matter candidates and mechanisms that generate the observed similarity between dark and visible matter densities.

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

The paper reviews models in which a new strongly-coupled gauge interaction confines at low energies, forming a dark sector separate from the Standard Model. These models yield stable dark matter particles in the form of dark mesons, baryons, and glueballs, whose properties arise from the same strong dynamics that govern ordinary hadrons. The review shows how such sectors supply both production mechanisms for the dark matter abundance and discrete symmetries that protect its stability. It maps out correlated signals across direct detection, indirect detection, astrophysical observations, and collider searches. A reader would care because these constructions address the abundance similarity puzzle while opening multiple experimental avenues from a small number of new ingredients.

Core claim

The central claim is that theories with confining dark sectors—new non-Abelian gauge interactions that become strong at low energies—lead to a variety of stable dark matter candidates including dark mesons, baryons, and glueballs, along with mechanisms for generating their abundance and explaining the similarity between dark and visible matter densities. These models also predict correlated signals in multiple experimental channels.

What carries the argument

Confining dark sectors realized by new strongly-coupled non-Abelian gauge interactions, which produce composite states (dark mesons, baryons, glueballs) and discrete symmetries that ensure stability while supplying abundance-generating processes.

If this is right

  • Dark matter need not be elementary but can be composite bound states whose spectrum is calculable from the new gauge dynamics.
  • The similarity between visible and dark matter densities can arise from shared production mechanisms or symmetry relations without additional tuning.
  • Signals in direct detection, colliders, and indirect searches become correlated, so a signal in one channel predicts the strength of signals in others.
  • The same framework can address multiple Standard Model puzzles simultaneously through the new gauge sector.
  • Calculational tools developed for ordinary QCD can be adapted to predict dark sector observables in different coupling regimes.

Where Pith is reading between the lines

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

  • If the framework holds, precision measurements of the dark matter density ratio could directly constrain the new gauge coupling and confinement scale.
  • Hidden valley scenarios at colliders would then be reinterpreted as concrete realizations of confining dark sectors rather than generic hidden sectors.
  • Astrophysical probes of dark matter self-interactions could test the composite nature of the candidates without requiring direct production.
  • The approach suggests that solving the abundance similarity puzzle may simultaneously resolve questions about dark matter stability and detection rates.

Load-bearing premise

That unifying features and calculational techniques apply across the various regimes of the theoretical landscape of confining dark sectors.

What would settle it

A dark matter particle discovered whose mass, spin, and interaction strengths cannot be realized as any composite state of a confining non-Abelian gauge theory, while the cosmic density ratio between dark and visible matter remains unexplained by other means.

Figures

Figures reproduced from arXiv: 2606.30760 by Austin Batz, Graham D. Kribs, Pouya Asadi.

Figure 1
Figure 1. Figure 1: Overview of motivations and common features of confining dark sectors. They can be used to solve a variety of theoretical puzzles, and the rich dark hadron spectrum leads to opportunities in theory modeling, exciting experimental signatures, and various naturally stable DM candidates. While the space of theories and applications is vast, commonalities in analysis methods and correlations among experimental… view at source ↗
Figure 2
Figure 2. Figure 2: Overview of some portal interactions that can connect the dark partons to the SM. Crossed dots denote where there may be higher-dimensional operators or mixings inserted. remainder of this section, we focus on the DM candidate as the categorization principle, and each of the other aforementioned schemes is addressed in the following sections. 2.1 Dark Baryons One of the few things we know about the nature … view at source ↗
Figure 3
Figure 3. Figure 3: Different phases of heavy dark quarks (black dots) being trapped in pockets of the deconfined phase (light purple) as the phase transition to the confined phase (dark purple) proceeds. In every single pocket (second row), dark quarks eventually recouple and the pocket shrinks, go through both annihilation and dark baryon DM (orange) formation. Eventually, only a small fraction of quarks in each pocket surv… view at source ↗
Figure 4
Figure 4. Figure 4: Schematic examples of common mediators enabling confined DM to scatter off SM nuclei. scalar technibaryon DM first occurs through the charge-radius interaction. A general low￾energy framework for constraining electromagnetic form factors of DM was developed in Ref. [246]. This analysis provided phenomenological estimates for the electromagnetic form factors for magnetic and electric dipoles, anapole moment… view at source ↗
Figure 5
Figure 5. Figure 5: Overview of some portal interactions that can connect dark hadrons either directly or indirectly to the SM, focusing on those relevant to collider phenomenology. Crossed dots denote where there may be higher-dimensional operators or mixings inserted. a chiral anomaly being produced via gluon-gluon or vector boson fusion [47, 91, 337, 338]. A chiral anomaly can also produce a single πD in association with a… view at source ↗
Figure 6
Figure 6. Figure 6: Sketch of mass scale regimes for collider phenomenology in terms of the dark quark mass mq and the dark sector confinement scale ΛD. The characteristic scale of the hard interaction Q is held fixed in the plot, though it can vary event-by-event due to parton distribution functions. The boundaries between regions are blurry and carry some implicit dependence on details such as flavor structure. When mq and … view at source ↗
Figure 7
Figure 7. Figure 7: Sketches of how various exotic/long-lived particle collider signatures would look inside the detector, similar to those in Refs. [481, 482]. Solid blue lines denote visible particles (which in some cases must be charged when tracking is essential), dashed black lines denote invisible particles, and dots denote decay vertices. 7 Calculating at Strong Coupling One of the major difficulties in theories involv… view at source ↗
read the original abstract

We review theories with confining dark sectors and their implications for dark matter, cosmology, phenomenology, and unsolved Standard Model puzzles. Models with new strongly-coupled non-Abelian gauge interactions can lead to a variety of dark matter candidates (dark mesons, baryons, glueballs, etc.), as well as mechanisms to generate its abundance and symmetries that explain its stability. There are also many potential discovery channels, including direct detection, indirect detection, astrophysical observables, and colliders, as well as correlations between different experiments. We compile a broad conceptual overview of the literature on this topic, aimed at both theorists looking for which questions remain unanswered and experimentalists looking for novel search opportunities. While the theoretical landscape is vast, there are both unifying features and calculational techniques that apply to various regimes. We particularly highlight applications to explaining the similarity of visible and dark matter energy densities, i.e. the $abundance~similarity~puzzle$. We advocate further exploration of this class of theories in the effort to uncover physics beyond the Standard Model.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. This manuscript reviews theories with confining dark sectors arising from new strongly-coupled non-Abelian gauge interactions. It surveys dark matter candidates including dark mesons, baryons, and glueballs; mechanisms for generating the dark matter abundance; symmetries ensuring stability; and discovery channels spanning direct detection, indirect detection, astrophysical observables, and colliders. The review compiles existing literature, notes correlations between observables, and particularly emphasizes applications to the visible-dark matter abundance similarity puzzle, while identifying unifying features and calculational techniques across regimes.

Significance. If the literature compilation is accurate and reasonably comprehensive, the review provides a useful conceptual map for theorists seeking open questions and for experimentalists identifying novel search strategies. It consolidates a broad class of models under a common framework without introducing new primary calculations.

minor comments (2)
  1. [Abstract] Abstract, final paragraph: the claim that 'unifying features and calculational techniques' apply across regimes is stated at a high level; a brief illustrative example or reference to a specific section would strengthen the point for readers.
  2. [Abstract] The manuscript title and abstract use 'Rich Phenomenology from Simple Ingredients'; consider adding a short footnote or sentence clarifying the scope of 'simple ingredients' (e.g., minimal gauge groups and matter content) to avoid ambiguity.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of the manuscript, including the recognition of its value as a conceptual map for theorists and experimentalists, and for the recommendation to accept. We are pleased that the review is viewed as consolidating the literature on confining dark sectors without introducing new primary calculations.

Circularity Check

0 steps flagged

No significant circularity identified

full rationale

This is a review paper that compiles and surveys existing literature on confining dark sectors, without presenting original derivations, predictions, equations, or fitted results. The abstract explicitly frames the work as a 'broad conceptual overview of the literature' aimed at highlighting open questions and search opportunities, with no load-bearing claims that reduce to self-definition, fitted inputs renamed as predictions, or self-citation chains. No derivation chain exists to inspect, so the paper is self-contained as a literature compilation against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

As a review the paper introduces no new free parameters, axioms, or invented entities; it summarizes models already present in the cited literature.

pith-pipeline@v0.9.1-grok · 5714 in / 998 out tokens · 31133 ms · 2026-07-01T01:50:42.759981+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

300 extracted references · 163 linked inside Pith

  1. [1]

    Dark Matter,

    M. Cirelli, A. Strumia, and J. Zupan, “Dark Matter,”arXiv:2406.01705 [hep-ph]. 3

  2. [2]

    Cosmological Lower Bound on Heavy Neutrino Masses,

    B. W. Lee and S. Weinberg, “Cosmological Lower Bound on Heavy Neutrino Masses,”Phys. Rev. Lett.39(1977) 165–168. 3

  3. [3]

    Cosmology of the Invisible Axion,

    J. Preskill, M. B. Wise, and F. Wilczek, “Cosmology of the Invisible Axion,”Phys. Lett. B120(1983) 127–132. 3

  4. [4]

    The Waning of the WIMP: Endgame?,

    G. Arcadi, D. Cabo-Almeida, M. Dutra, P. Ghosh, M. Lindner, Y. Mambrini, J. P. Neto, M. Pierre, S. Profumo, and F. S. Queiroz, “The Waning of the WIMP: Endgame?,”Eur. Phys. J. C85(2025) no. 2, 152,arXiv:2403.15860 [hep-ph]. 3

  5. [5]

    Searching for the QCD Dark Matter Axion,

    M. Baryakhtar, L. Rosenberg, and G. Rybka, “Searching for the QCD Dark Matter Axion,”arXiv:2504.10607 [hep-ex]. 3

  6. [6]

    TECHNOCOSMOLOGY: COULD A TECHNIBARYON EXCESS PROVIDE A ’NATURAL’ MISSING MASS CANDIDATE?,

    S. Nussinov, “TECHNOCOSMOLOGY: COULD A TECHNIBARYON EXCESS PROVIDE A ’NATURAL’ MISSING MASS CANDIDATE?,”Phys. Lett. B165 (1985) 55–58. 3, 8

  7. [7]

    TECHNICOLOR COSMOLOGY,

    R. S. Chivukula and T. P. Walker, “TECHNICOLOR COSMOLOGY,”Nucl. Phys. B329(1990) 445–463. 3, 16

  8. [8]

    Electroweak Fermion Number Violation and the Production of Stable Particles in the Early Universe,

    S. M. Barr, R. S. Chivukula, and E. Farhi, “Electroweak Fermion Number Violation and the Production of Stable Particles in the Early Universe,”Phys. Lett. B241 (1990) 387–391. 3

  9. [9]

    Detecting technibaryon dark matter,

    J. Bagnasco, M. Dine, and S. D. Thomas, “Detecting technibaryon dark matter,” Phys. Lett. B320(1994) 99–104,arXiv:hep-ph/9310290. 3, 9, 20

  10. [10]

    Towards working technicolor: Effective theories and dark matter,

    S. B. Gudnason, C. Kouvaris, and F. Sannino, “Towards working technicolor: Effective theories and dark matter,”Phys. Rev. D73(2006) 115003, arXiv:hep-ph/0603014. 3, 9

  11. [11]

    Dark Matter from new Technicolor Theories,

    S. B. Gudnason, C. Kouvaris, and F. Sannino, “Dark Matter from new Technicolor Theories,”Phys. Rev. D74(2006) 095008,arXiv:hep-ph/0608055. 3, 9

  12. [12]

    Ultra Minimal Technicolor and its Dark Matter TIMP,

    T. A. Ryttov and F. Sannino, “Ultra Minimal Technicolor and its Dark Matter TIMP,”Phys. Rev. D78(2008) 115010,arXiv:0809.0713 [hep-ph]. 3, 9

  13. [13]

    Technicolor Dark Matter,

    R. Foadi, M. T. Frandsen, and F. Sannino, “Technicolor Dark Matter,”Phys. Rev. D 80(2009) 037702,arXiv:0812.3406 [hep-ph]. 3

  14. [14]

    Secluded WIMP Dark Matter,

    M. Pospelov, A. Ritz, and M. B. Voloshin, “Secluded WIMP Dark Matter,”Phys. Lett. B662(2008) 53–61,arXiv:0711.4866 [hep-ph]. 3

  15. [15]

    Atomic Dark Matter,

    D. E. Kaplan, G. Z. Krnjaic, K. R. Rehermann, and C. M. Wells, “Atomic Dark Matter,”JCAP05(2010) 021,arXiv:0909.0753 [hep-ph]. 4

  16. [16]

    LargeN-ightmare Dark Matter,

    L. Morrison, S. Profumo, and D. J. Robinson, “LargeN-ightmare Dark Matter,” JCAP05(2021) 058,arXiv:2010.03586 [hep-ph]. 4, 14, 15, 45 50

  17. [17]

    Composite Scalar Dark Matter,

    M. Frigerio, A. Pomarol, F. Riva, and A. Urbano, “Composite Scalar Dark Matter,” JHEP07(2012) 015,arXiv:1204.2808 [hep-ph]. 4

  18. [18]

    Composite Dark Matter and LHC Interplay,

    D. Marzocca and A. Urbano, “Composite Dark Matter and LHC Interplay,”JHEP 07(2014) 107,arXiv:1404.7419 [hep-ph]. 4

  19. [19]

    The Unnatural Composite Higgs,

    J. Barnard, T. Gherghetta, T. S. Ray, and A. Spray, “The Unnatural Composite Higgs,”JHEP01(2015) 067,arXiv:1409.7391 [hep-ph]. 4

  20. [20]

    A Dark matter candidate with new strong interactions,

    T. Banks, J. D. Mason, and D. O’Neil, “A Dark matter candidate with new strong interactions,”Phys. Rev. D72(2005) 043530,arXiv:hep-ph/0506015. 4, 46

  21. [21]

    Composite messenger baryon as a cold dark matter,

    K. Hamaguchi, S. Shirai, and T. T. Yanagida, “Composite messenger baryon as a cold dark matter,”Phys. Lett. B654(2007) 110–112,arXiv:0707.2463 [hep-ph]. 4, 46

  22. [22]

    Decaying Dark Matter Baryons in a Composite Messenger Model,

    K. Hamaguchi, E. Nakamura, S. Shirai, and T. T. Yanagida, “Decaying Dark Matter Baryons in a Composite Messenger Model,”Phys. Lett. B674(2009) 299–302, arXiv:0811.0737 [hep-ph]. 4, 46

  23. [23]

    Cosmic Signals from the Hidden Sector,

    J. Mardon, Y. Nomura, and J. Thaler, “Cosmic Signals from the Hidden Sector,” Phys. Rev. D80(2009) 035013,arXiv:0905.3749 [hep-ph]. 4, 46

  24. [24]

    Low-Scale Gauge Mediation and Composite Messenger Dark Matter,

    K. Hamaguchi, E. Nakamura, S. Shirai, and T. T. Yanagida, “Low-Scale Gauge Mediation and Composite Messenger Dark Matter,”JHEP04(2010) 119, arXiv:0912.1683 [hep-ph]. 4, 46

  25. [25]

    A COMPOSITE INVISIBLE AXION,

    J. E. Kim, “A COMPOSITE INVISIBLE AXION,”Phys. Rev. D31(1985) 1733. 4

  26. [26]

    Composite axion models and Planck scale physics,

    L. Randall, “Composite axion models and Planck scale physics,”Phys. Lett. B284 (1992) 77–80. 4

  27. [27]

    The Strong CP problem versus Planck scale physics,

    B. A. Dobrescu, “The Strong CP problem versus Planck scale physics,”Phys. Rev. D 55(1997) 5826–5833,arXiv:hep-ph/9609221. 4

  28. [28]

    Warped axions,

    T. Flacke, B. Gripaios, J. March-Russell, and D. Maybury, “Warped axions,”JHEP 01(2007) 061,arXiv:hep-ph/0611278. 4

  29. [29]

    Composite Accidental Axions,

    M. Redi and R. Sato, “Composite Accidental Axions,”JHEP05(2016) 104, arXiv:1602.05427 [hep-ph]. 4

  30. [30]

    Accidental Peccei-Quinn symmetry protected to arbitrary order,

    L. Di Luzio, E. Nardi, and L. Ubaldi, “Accidental Peccei-Quinn symmetry protected to arbitrary order,”Phys. Rev. Lett.119(2017) no. 1, 011801,arXiv:1704.01122 [hep-ph]. 4

  31. [31]

    A Composite Axion from a Supersymmetric Product Group,

    B. Lillard and T. M. P. Tait, “A Composite Axion from a Supersymmetric Product Group,”JHEP11(2017) 005,arXiv:1707.04261 [hep-ph]. 4

  32. [32]

    A High Quality Composite Axion,

    B. Lillard and T. M. P. Tait, “A High Quality Composite Axion,”JHEP11(2018) 199,arXiv:1811.03089 [hep-ph]. 4

  33. [33]

    A Holographic Perspective on the Axion Quality Problem,

    P. Cox, T. Gherghetta, and M. D. Nguyen, “A Holographic Perspective on the Axion Quality Problem,”JHEP01(2020) 188,arXiv:1911.09385 [hep-ph]. 4

  34. [34]

    A Composite Higgs with a Heavy Composite Axion,

    T. Gherghetta and M. D. Nguyen, “A Composite Higgs with a Heavy Composite Axion,”JHEP12(2020) 094,arXiv:2007.10875 [hep-ph]. 4 51

  35. [35]

    Chiral models of composite axions and accidental Peccei-Quinn symmetry,

    R. Contino, A. Podo, and F. Revello, “Chiral models of composite axions and accidental Peccei-Quinn symmetry,”JHEP04(2022) 180,arXiv:2112.09635 [hep-ph]. 4

  36. [36]

    High-quality composite Pati-Salam axion,

    T. Gherghetta, H. Murayama, and P. Qu´ ılez, “High-quality composite Pati-Salam axion,”Phys. Rev. D112(2025) no. 9, 095036,arXiv:2505.08866 [hep-ph]. 4

  37. [37]

    A High-Quality Axion from Exact SUSY Chiral Dynamics,

    T. Gherghetta, H. Murayama, B. Noether, and P. Qu´ ılez, “A High-Quality Axion from Exact SUSY Chiral Dynamics,”arXiv:2508.21813 [hep-ph]. 4, 46

  38. [38]

    Axion quality problem: keep calm and baryon,

    P. Agrawal, A. Hook, V. Loladze, and M. Reig, “Axion quality problem: keep calm and baryon,”JHEP03(2026) 041,arXiv:2510.07366 [hep-ph]. 4

  39. [39]

    Towards a post-inflationary composite axion model,

    A. Azatov, M. Mahdi Khalil, and M. Suzuki, “Towards a post-inflationary composite axion model,”JHEP03(2026) 143,arXiv:2510.18538 [hep-ph]. 4

  40. [40]

    Axiverse Baryogenesis,

    P. Asadi, D. Cyncynates, and S. Gori, “Axiverse Baryogenesis,”arXiv:2511.15794 [hep-ph]. 4

  41. [41]

    Hierarchies without symmetries from extra dimensions,

    N. Arkani-Hamed and M. Schmaltz, “Hierarchies without symmetries from extra dimensions,”Phys. Rev. D61(2000) 033005,arXiv:hep-ph/9903417. 4

  42. [42]

    Fermion masses, mixings and proton decay in a Randall-Sundrum model,

    S. J. Huber and Q. Shafi, “Fermion masses, mixings and proton decay in a Randall-Sundrum model,”Phys. Lett. B498(2001) 256–262, arXiv:hep-ph/0010195. 4

  43. [43]

    A Model of Lepton Masses from a Warped Extra Dimension,

    C. Csaki, C. Delaunay, C. Grojean, and Y. Grossman, “A Model of Lepton Masses from a Warped Extra Dimension,”JHEP10(2008) 055,arXiv:0806.0356 [hep-ph]. 4

  44. [44]

    Implications of a Light Higgs in Composite Models,

    M. Redi and A. Tesi, “Implications of a Light Higgs in Composite Models,”JHEP10 (2012) 166,arXiv:1205.0232 [hep-ph]. 4

  45. [45]

    Violation of CP Invariance, C asymmetry, and baryon asymmetry of the universe,

    A. D. Sakharov, “Violation of CP Invariance, C asymmetry, and baryon asymmetry of the universe,”Pisma Zh. Eksp. Teor. Fiz.5(1967) 32–35. 5

  46. [46]

    Confined hidden vector dark matter,

    T. Hambye and M. H. G. Tytgat, “Confined hidden vector dark matter,”Phys. Lett. B683(2010) 39–41,arXiv:0907.1007 [hep-ph]. 7

  47. [47]

    Accidental Composite Dark Matter,

    O. Antipin, M. Redi, A. Strumia, and E. Vigiani, “Accidental Composite Dark Matter,”JHEP07(2015) 039,arXiv:1503.08749 [hep-ph]. 7, 11, 16, 22, 24, 33, 45

  48. [48]

    Thermal history of composite dark matter,

    N. A. Dondi, F. Sannino, and J. Smirnov, “Thermal history of composite dark matter,”Phys. Rev. D101(2020) no. 10, 103010,arXiv:1905.08810 [hep-ph]. 7, 31

  49. [49]

    Surveying the theory space of pion dark matter,

    A. Alfano, N. Evans, S. Kulkarni, and W. Porod, “Surveying the theory space of pion dark matter,”arXiv:2509.04892 [hep-ph]. 7

  50. [50]

    Echoes of a hidden valley at hadron colliders,

    M. J. Strassler and K. M. Zurek, “Echoes of a hidden valley at hadron colliders,” Phys. Lett. B651(2007) 374–379,arXiv:hep-ph/0604261. 7, 32

  51. [51]

    Light Asymmetric Dark Matter on the Lattice: SU(2) Technicolor with Two Fundamental Flavors,

    R. Lewis, C. Pica, and F. Sannino, “Light Asymmetric Dark Matter on the Lattice: SU(2) Technicolor with Two Fundamental Flavors,”Phys. Rev. D85(2012) 014504, arXiv:1109.3513 [hep-ph]. 9, 43 52

  52. [52]

    The LargeNlimit of superconformal field theories and supergravity,

    J. M. Maldacena, “The LargeNlimit of superconformal field theories and supergravity,”Adv. Theor. Math. Phys.2(1998) 231–252,arXiv:hep-th/9711200. 9

  53. [53]

    Anti de Sitter space and holography,

    E. Witten, “Anti de Sitter space and holography,”Adv. Theor. Math. Phys.2(1998) 253–291,arXiv:hep-th/9802150. 9

  54. [54]

    Holography and phenomenology,

    N. Arkani-Hamed, M. Porrati, and L. Randall, “Holography and phenomenology,” JHEP08(2001) 017,arXiv:hep-th/0012148. 9

  55. [55]

    Warped unification, proton stability and dark matter,

    K. Agashe and G. Servant, “Warped unification, proton stability and dark matter,” Phys. Rev. Lett.93(2004) 231805,arXiv:hep-ph/0403143. 9

  56. [56]

    Electroweak symmetry breaking and cold dark matter from strongly interacting hidden sector,

    T. Hur, D.-W. Jung, P. Ko, and J. Y. Lee, “Electroweak symmetry breaking and cold dark matter from strongly interacting hidden sector,”Phys. Lett. B696(2011) 262–265,arXiv:0709.1218 [hep-ph]. 9, 10

  57. [57]

    Dynamical generation of the weak and Dark Matter scale,

    T. Hambye and A. Strumia, “Dynamical generation of the weak and Dark Matter scale,”Phys. Rev. D88(2013) 055022,arXiv:1306.2329 [hep-ph]. 9

  58. [58]

    Phenomenology of Induced Electroweak Symmetry Breaking,

    S. Chang, J. Galloway, M. Luty, E. Salvioni, and Y. Tsai, “Phenomenology of Induced Electroweak Symmetry Breaking,”JHEP03(2015) 017,arXiv:1411.6023 [hep-ph]. 9

  59. [59]

    Quirky Composite Dark Matter,

    G. D. Kribs, T. S. Roy, J. Terning, and K. M. Zurek, “Quirky Composite Dark Matter,”Phys. Rev. D81(2010) 095001,arXiv:0909.2034 [hep-ph]. 9, 16, 23, 31, 39, 41

  60. [60]

    Weakly Interacting Stable Pions,

    Y. Bai and R. J. Hill, “Weakly Interacting Stable Pions,”Phys. Rev. D82(2010) 111701,arXiv:1005.0008 [hep-ph]. 9, 10 [61]Lattice Strong Dynamics (LSD)Collaboration, T. Appelquistet al., “Lattice Calculation of Composite Dark Matter Form Factors,”Phys. Rev. D88(2013) no. 1, 014502,arXiv:1301.1693 [hep-ph]. 9, 22, 42 [62]LSDCollaboration, T. Appelquistet al...

  61. [61]

    Dynamical generation of the weak and Dark Matter scales from strong interactions,

    O. Antipin, M. Redi, and A. Strumia, “Dynamical generation of the weak and Dark Matter scales from strong interactions,”JHEP01(2015) 157,arXiv:1410.1817 [hep-ph]. 9, 11, 14, 45

  62. [62]

    Detecting Stealth Dark Matter Directly through Electromagnetic Polarizability,

    T. Appelquistet al., “Detecting Stealth Dark Matter Directly through Electromagnetic Polarizability,”Phys. Rev. Lett.115(2015) no. 17, 171803, arXiv:1503.04205 [hep-ph]. 9, 22, 43

  63. [63]

    Stealth Dark Matter: Dark scalar baryons through the Higgs portal,

    T. Appelquistet al., “Stealth Dark Matter: Dark scalar baryons through the Higgs portal,”Phys. Rev. D92(2015) no. 7, 075030,arXiv:1503.04203 [hep-ph]. 9, 14, 23, 33, 42

  64. [64]

    A scenario of heavy but visible baryonic dark matter,

    R. Huo, S. Matsumoto, Y.-L. Sming Tsai, and T. T. Yanagida, “A scenario of heavy but visible baryonic dark matter,”JHEP09(2016) 162,arXiv:1506.06929 [hep-ph]. 9, 10 53

  65. [65]

    Dark Matter as a weakly coupled Dark Baryon,

    A. Mitridate, M. Redi, J. Smirnov, and A. Strumia, “Dark Matter as a weakly coupled Dark Baryon,”JHEP10(2017) 210,arXiv:1707.05380 [hep-ph]. 9, 10, 11, 14, 23, 24, 30, 42, 45

  66. [66]

    Composite Dark Matter from Strongly-Interacting Chiral Dynamics,

    R. Contino, A. Podo, and F. Revello, “Composite Dark Matter from Strongly-Interacting Chiral Dynamics,”JHEP02(2021) 091,arXiv:2008.10607 [hep-ph]. 9, 10

  67. [67]

    Hyperstealth dark matter and long-lived particles,

    G. T. Fleming, G. D. Kribs, E. T. Neil, D. Schaich, and P. M. Vranas, “Hyperstealth dark matter and long-lived particles,”Phys. Rev. D112(2025) no. 7, 075004, arXiv:2412.14540 [hep-ph]. 9, 14, 24, 45

  68. [68]

    Composite Dark Matter and a horizontal symmetry,

    A. Carvunis, D. Guadagnoli, M. Reboud, and P. Stangl, “Composite Dark Matter and a horizontal symmetry,”JHEP02(2021) 056,arXiv:2007.11931 [hep-ph]. 9

  69. [69]

    Gauged Flavour for Asymmetric Dark Matter,

    M. Blennow, E. Fernandez-Martinez, D. Garcia-Garcia, and J. M. Lizana, “Gauged Flavour for Asymmetric Dark Matter,”arXiv:2605.20336 [hep-ph]. 9, 32

  70. [70]

    Challenges for models with composite states,

    J. M. Cline, W. Huang, and G. D. Moore, “Challenges for models with composite states,”Phys. Rev. D94(2016) no. 5, 055029,arXiv:1607.07865 [hep-ph]. 9

  71. [71]

    Colored Dark Matter,

    V. De Luca, A. Mitridate, M. Redi, J. Smirnov, and A. Strumia, “Colored Dark Matter,”Phys. Rev. D97(2018) no. 11, 115024,arXiv:1801.01135 [hep-ph]. 9, 25, 30

  72. [72]

    Baryons, multihadron systems, and composite dark matter in nonrelativistic QCD,

    B. Assi and M. L. Wagman, “Baryons, multihadron systems, and composite dark matter in nonrelativistic QCD,”Phys. Rev. D108(2023) no. 9, 096004, arXiv:2305.01685 [hep-ph]. 10, 42

  73. [73]

    TeV symmetry and the little hierarchy problem,

    H.-C. Cheng and I. Low, “TeV symmetry and the little hierarchy problem,”JHEP 09(2003) 051,arXiv:hep-ph/0308199. 10

  74. [74]

    KK Parity in Warped Extra Dimension,

    K. Agashe, A. Falkowski, I. Low, and G. Servant, “KK Parity in Warped Extra Dimension,”JHEP04(2008) 027,arXiv:0712.2455 [hep-ph]. 10

  75. [75]

    Probing Dark Forces and Light Hidden Sectors at Low-Energy e+e- Colliders,

    R. Essig, P. Schuster, and N. Toro, “Probing Dark Forces and Light Hidden Sectors at Low-Energy e+e- Colliders,”Phys. Rev. D80(2009) 015003,arXiv:0903.3941 [hep-ph]. 10

  76. [76]

    Pionic Dark Matter,

    S. Bhattacharya, B. Meli´ c, and J. Wudka, “Pionic Dark Matter,”JHEP02(2014) 115,arXiv:1307.2647 [hep-ph]. 10

  77. [77]

    Composite strongly interacting dark matter,

    J. M. Cline, Z. Liu, G. D. Moore, and W. Xue, “Composite strongly interacting dark matter,”Phys. Rev. D90(2014) no. 1, 015023,arXiv:1312.3325 [hep-ph]. 10, 32

  78. [78]

    Model for Thermal Relic Dark Matter of Strongly Interacting Massive Particles,

    Y. Hochberg, E. Kuflik, H. Murayama, T. Volansky, and J. G. Wacker, “Model for Thermal Relic Dark Matter of Strongly Interacting Massive Particles,”Phys. Rev. Lett.115(2015) no. 2, 021301,arXiv:1411.3727 [hep-ph]. 10, 14

  79. [79]

    Light Chiral Dark Sector,

    K. Harigaya and Y. Nomura, “Light Chiral Dark Sector,”Phys. Rev. D94(2016) no. 3, 035013,arXiv:1603.03430 [hep-ph]. 10

  80. [80]

    Impeded Dark Matter,

    J. Kopp, J. Liu, T. R. Slatyer, X.-P. Wang, and W. Xue, “Impeded Dark Matter,” JHEP12(2016) 033,arXiv:1609.02147 [hep-ph]. 10 54

Showing first 80 references.