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arxiv: 2606.06645 · v1 · pith:F3KSMU7Tnew · submitted 2026-06-04 · ✦ hep-ph

micrOMEGAs 7: Beyond standard cosmology

Pith reviewed 2026-06-28 00:11 UTC · model grok-4.3

classification ✦ hep-ph
keywords dark matter relic densityBoltzmann equationsnon-standard cosmologyHubble expansion rateearly matter dominationkinationlow-temperature reheating
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0 comments X

The pith

micrOMEGAs7 now solves the Boltzmann equations with arbitrary user modifications to the Hubble rate and entropy to compute relic densities outside standard radiation-dominated cosmology.

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

The paper presents a major update that generalizes the equations governing dark matter number density evolution. It lets users specify changes to the expansion rate, entropy production, and late-time particle decays that inject dark matter. These changes make it possible to calculate the final dark matter abundance after periods of early matter domination, low-temperature reheating, or kination. The same release also refines annihilation calculations for sub-GeV dark matter and adds several new experimental bounds.

Core claim

By allowing user-defined modifications to the Hubble expansion rate, entropy evolution, and non-thermal dark matter production from late-decaying components, the updated code solves the Boltzmann equations beyond the standard radiation-dominated universe and thereby computes relic densities in low-temperature reheating, early matter domination, and kination scenarios.

What carries the argument

A generalized Boltzmann solver that accepts arbitrary user-specified functions for the Hubble parameter and entropy density while tracking non-thermal production terms.

If this is right

  • Relic density results become available for any early-universe expansion history supplied by the user.
  • Non-thermal dark matter injection from late decays can be included without rewriting the core equations.
  • Direct detection and indirect detection rates can be evaluated consistently with the new cosmological histories.
  • Updated spectra for light-meson final states improve predictions for sub-GeV dark matter annihilation.

Where Pith is reading between the lines

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

  • The same interface could be used to explore dark matter production tied to specific models of entropy injection during the QCD phase transition.
  • Users might link the modified expansion histories to constraints from primordial gravitational waves or baryon asymmetry.
  • The framework opens a route to systematic scans over reheating temperatures while keeping the particle physics model fixed.

Load-bearing premise

The numerical integration remains stable and accurate when the Hubble rate and entropy are replaced by arbitrary user functions that differ strongly from standard radiation domination.

What would settle it

An independent analytic or numerical calculation of the relic density for a concrete early-matter-domination scenario with given reheating temperature and decay width that matches or deviates from the code output within stated precision.

read the original abstract

We present micrOMEGAs7, a major upgrade of the micrOMEGAs package for the computation of dark matter observables in generic models. This release introduces a generalized treatment of the Boltzmann equations, allowing for user-defined modifications of the Hubble expansion rate, entropy evolution, and non-thermal dark matter production from late-decaying cosmological components, thereby extending the framework beyond the standard radiation-dominated cosmology. The relic density can now be computed in scenarios such as low-temperature reheating, early matter domination, and kination. The new version also improves the treatment of sub-GeV dark matter, in particular annihilation into light mesons through scalar mediators, and provides updated spectra for indirect detection. Several experimental and observational constraints have been implemented or revised, including CMB bounds from Planck on energy injection during recombination and Fermi-LAT limits from dwarf spheroidal galaxies. For direct detection, a recast of recent LZ results has been included, and the code now takes into account effective electromagnetic couplings of spin-$1/2$ and spin-1 dark matter. Collider observables have also been extended through the implementation of CMS dilepton resonance constraints on $Z'$ mediators. Additional improvements include a more flexible treatment of effective relativistic degrees of freedom and an updated LHAPDF interface.

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

1 major / 0 minor

Summary. The manuscript describes the release of micrOMEGAs 7, which extends the micrOMEGAs package with a generalized treatment of the Boltzmann equations. This allows user-defined modifications to the Hubble expansion rate, entropy evolution, and non-thermal dark matter production, enabling relic density computations in non-standard cosmologies such as low-temperature reheating, early matter domination, and kination. Additional updates cover sub-GeV DM annihilation into light mesons, updated indirect detection spectra, revised constraints from Planck, Fermi-LAT, LZ, and CMS, a more flexible treatment of relativistic degrees of freedom, and an updated LHAPDF interface.

Significance. If the numerical implementation is robust, the extension to non-standard cosmologies would be significant for dark matter phenomenology, as it permits calculations in scenarios where the standard radiation-dominated expansion does not apply and could affect relic density predictions and experimental interpretations. The updated constraints and sub-GeV improvements would further increase the package's utility for model scans and data comparison.

major comments (1)
  1. [Abstract] Abstract: the central claim that relic densities can now be reliably computed via the generalized Boltzmann solver in scenarios such as early matter domination and kination is not supported by any validation tests, analytic limit comparisons, convergence checks, or stability analysis for arbitrary user-specified H(t) or entropy modifications; this is load-bearing for the advertised functionality.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their detailed review and for recognizing the potential significance of the generalized Boltzmann solver in micrOMEGAs 7. We address the single major comment below.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the central claim that relic densities can now be reliably computed via the generalized Boltzmann solver in scenarios such as early matter domination and kination is not supported by any validation tests, analytic limit comparisons, convergence checks, or stability analysis for arbitrary user-specified H(t) or entropy modifications; this is load-bearing for the advertised functionality.

    Authors: We agree that explicit validation strengthens the central claim. The current manuscript presents the implementation and illustrates its use through example scenarios, but does not include dedicated analytic-limit comparisons, convergence tests, or stability analysis for arbitrary user-specified modifications. In the revised version we will add a new subsection (or appendix) containing: (i) recovery of the standard radiation-dominated result for H(t) and entropy evolution matching the usual case, (ii) comparison against known analytic solutions for early matter domination and kination, and (iii) numerical convergence and stability checks for representative user-defined H(t) and entropy profiles. These additions will be referenced from the abstract. revision: yes

Circularity Check

0 steps flagged

No circularity: software release note with no derivation chain

full rationale

The document is a release note describing added numerical functionality in micrOMEGAs7 for generalized Boltzmann solvers under user-specified H(t), entropy, and non-thermal production. No theoretical derivation, fitted parameter, or prediction is presented that could reduce to its own inputs by construction. The text lists features and constraints implemented but contains no equations, ansatze, or self-citations invoked as load-bearing uniqueness theorems. The central claim is simply that the code now supports these extensions; correctness is an implementation and validation matter outside the scope of circularity analysis. No steps meet the criteria for any enumerated circularity pattern.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

The document is a software update note; no free parameters, axioms, or invented entities are introduced in a scientific derivation sense.

pith-pipeline@v0.9.1-grok · 5779 in / 1116 out tokens · 19796 ms · 2026-06-28T00:11:24.634936+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

81 extracted references · 2 canonical work pages

  1. [1]

    B´ elanger, F

    G. B´ elanger, F. Boudjema, A. Pukhov and A. Semenov,MicrOMEGAs: A Program for calculating the relic density in the MSSM,Comput. Phys. Commun.149(2002) 103 [hep-ph/0112278]

  2. [2]

    Gondolo, J

    P. Gondolo, J. Edsj¨ o, P. Ullio, L. Bergstrom, M. Schelke and E.A. Baltz,DarkSUSY: – 24 – 100 101 102 103 104 105 106 107 a 101 102 103 104 105 106 107 108 109 z HSM = 0 HSM = 10 3HI z Figure 7:z χ as a function of the scale factor for two different values ofH SM = 0 or HSM = 10−3Hϕ whenα= 3/8,w= 0. The parameters of theZ ′ portal model are chosen as in ...

  3. [3]

    B´ elanger, F

    G. B´ elanger, F. Boudjema, A. Pukhov and A. Semenov,MicrOMEGAs 2.0: A Program to calculate the relic density of dark matter in a generic model,Comput. Phys. Commun.176 (2007) 367 [hep-ph/0607059]

  4. [4]

    Backovi´ c, K

    M. Backovi´ c, K. Kong and M. McCaskey,MadDM v.1.0: Computation of Dark Matter Relic Abundance Using MadGraph5,Physics of the Dark Universe5-6(2014) 18 [1308.4955]

  5. [5]

    Ambrogi, C

    F. Ambrogi, C. Arina, M. Backovi´ c, J. Heisig, F. Maltoni, L. Mantani et al.,MadDM v.3.0: a Comprehensive Tool for Dark Matter Studies,Phys. Dark Univ.24(2019) 100249 [1804.00044]

  6. [6]

    Arbey, F

    A. Arbey, F. Mahmoudi and G. Robbins,SuperIso Relic v4: A program for calculating dark matter and flavour physics observables in Supersymmetry,Comput. Phys. Commun.239 (2019) 238 [1806.11489]

  7. [7]

    Bringmann, J

    T. Bringmann, J. Edsj¨ o, P. Gondolo, P. Ullio and L. Bergstr¨ om,DarkSUSY 6 : An Advanced Tool to Compute Dark Matter Properties Numerically,JCAP07(2018) 033 [1802.03399]

  8. [8]

    Palmiotto, A

    M. Palmiotto, A. Arbey and F. Mahmoudi,DarkPACK: A modular software to compute BSM squared amplitudes for particle physics and dark matter observables,Comput. Phys. Commun. 294(2024) 108905 [2211.10376]

  9. [9]

    Alguero, G

    G. Alguero, G. B´ elanger, F. Boudjema, S. Chakraborti, A. Goudelis, S. Kraml et al., micrOMEGAs 6.0: N-component dark matter,Comput. Phys. Commun.299(2024) 109133 [2312.14894]

  10. [10]

    Capucha, K

    R. Capucha, K. Elyaouti, M.M. M¨ uhlleitner, J. Plotnikov and R. Santos,RelExt: A New Dark Matter Tool for the Exploration of Dark Matter Models,Comput. Phys. Commun.320(2026) 109968 [2503.13087]

  11. [11]

    Giudice, E.W

    G.F. Giudice, E.W. Kolb and A. Riotto,Largest temperature of the radiation era and its cosmological implications,Phys. Rev. D64(2001) 023508 [hep-ph/0005123]

  12. [12]

    Fornengo, A

    N. Fornengo, A. Riotto and S. Scopel,Supersymmetric dark matter and the reheating temperature of the universe,Phys. Rev. D67(2003) 023514 [hep-ph/0208072]. – 25 –

  13. [13]

    Gelmini and P

    G.B. Gelmini and P. Gondolo,Neutralino with the right cold dark matter abundance in (almost) any supersymmetric model,Phys. Rev. D74(2006) 023510 [hep-ph/0602230]

  14. [14]

    Acharya, G

    B.S. Acharya, G. Kane, S. Watson and P. Kumar,A Non-thermal WIMP Miracle,Phys. Rev. D80(2009) 083529 [0908.2430]

  15. [15]

    G. Kane, K. Sinha and S. Watson,Cosmological Moduli and the Post-Inflationary Universe: A Critical Review,Int. J. Mod. Phys. D24(2015) 1530022 [1502.07746]

  16. [16]

    Zel’dovich,The Equation of State at Ultrahigh Densities and Its Relativistic Limitations, Zh

    Y.B. Zel’dovich,The Equation of State at Ultrahigh Densities and Its Relativistic Limitations, Zh. Eksp. Teor. Fiz.41(1961) 1609

  17. [17]

    Spokoiny,Deflationary universe scenario,Phys

    B. Spokoiny,Deflationary universe scenario,Phys. Lett. B315(1993) 40 [gr-qc/9306008]

  18. [18]

    Joyce,Electroweak Baryogenesis and the Expansion Rate of the Universe,Phys

    M. Joyce,Electroweak Baryogenesis and the Expansion Rate of the Universe,Phys. Rev. D55 (1997) 1875 [hep-ph/9606223]

  19. [19]

    Ferreira and M

    P.G. Ferreira and M. Joyce,Cosmology with a primordial scaling field,Phys. Rev. D58(1998) 023503 [astro-ph/9711102]

  20. [20]

    D’Eramo, N

    F. D’Eramo, N. Fern´ andez and S. Profumo,When the Universe Expands Too Fast: Relentless Dark Matter,JCAP05(2017) 012 [1703.04793]

  21. [21]

    Barman, P

    B. Barman, P. Ghosh, F.S. Queiroz and A.K. Saha,Scalar multiplet dark matter in a fast expanding Universe: Resurrection of the desert region,Phys. Rev. D104(2021) 015040 [2101.10175]

  22. [22]

    B´ elanger, N

    G. B´ elanger, N. Bernal, A. Goudelis and A. Pukhov,Kination and the Inert Doublet Model, 2512.15864

  23. [23]

    Turner,Coherent Scalar Field Oscillations in an Expanding Universe,Phys

    M.S. Turner,Coherent Scalar Field Oscillations in an Expanding Universe,Phys. Rev. D28 (1983) 1243

  24. [24]

    Slatyer,Indirect dark matter signatures in the cosmic dark ages

    T.R. Slatyer,Indirect dark matter signatures in the cosmic dark ages. I. Generalizing the bound on s-wave dark matter annihilation from Planck results,Phys. Rev. D93(2016) 023527 [1506.03811]

  25. [25]

    Calore, P.D

    F. Calore, P.D. Serpico and B. Zald´ ıvar,Dark matter constraints from dwarf galaxies: a data-driven analysis,JCAP10(2018) 029 [1803.05508]

  26. [26]

    ´Alvarez, F

    A. ´Alvarez, F. Calore, A. Genina, J. Read, P.D. Serpico and B. Zald´ ıvar,Dark matter constraints from dwarf galaxies with data-driven J-factors,JCAP09(2020) 004 [2002.01229]

  27. [27]

    B´ elanger, F

    G. B´ elanger, F. Boudjema, A. Goudelis, A. Pukhov and B. Zald´ ıvar,micrOMEGAs5.0 : Freeze-in,Comput. Phys. Commun.231(2018) 173 [1801.03509]

  28. [28]

    Sarkar,Big bang nucleosynthesis and physics beyond the standard model,Rept

    S. Sarkar,Big bang nucleosynthesis and physics beyond the standard model,Rept. Prog. Phys. 59(1996) 1493 [hep-ph/9602260]

  29. [29]

    Kawasaki, K

    M. Kawasaki, K. Kohri and N. Sugiyama,MeV scale reheating temperature and thermalization of neutrino background,Phys. Rev. D62(2000) 023506 [astro-ph/0002127]

  30. [30]

    Hannestad,What is the lowest possible reheating temperature?,Phys

    S. Hannestad,What is the lowest possible reheating temperature?,Phys. Rev. D70(2004) 043506 [astro-ph/0403291]

  31. [31]

    Barbieri, T

    N. Barbieri, T. Brinckmann, S. Gariazzo, M. Lattanzi, S. Pastor and O. Pisanti,Current Constraints on Cosmological Scenarios with Very Low Reheating Temperatures,Phys. Rev. Lett.135(2025) 181003 [2501.01369]

  32. [32]

    Bassett, S

    B.A. Bassett, S. Tsujikawa and D. Wands,Inflation dynamics and reheating,Rev. Mod. Phys. 78(2006) 537 [astro-ph/0507632]

  33. [33]

    Allahverdi, R

    R. Allahverdi, R. Brandenberger, F.-Y. Cyr-Racine and A. Mazumdar,Reheating in Inflationary Cosmology: Theory and Applications,Ann. Rev. Nucl. Part. Sci.60(2010) 27 [1001.2600]. – 26 –

  34. [34]

    Amin, M.P

    M.A. Amin, M.P. Hertzberg, D.I. Kaiser and J. Karouby,Nonperturbative Dynamics Of Reheating After Inflation: A Review,Int. J. Mod. Phys. D24(2014) 1530003 [1410.3808]

  35. [35]

    Lozanov,Lectures on Reheating after Inflation,1907.04402

    K.D. Lozanov,Lectures on Reheating after Inflation,1907.04402

  36. [36]

    Lozanov,Reheating After Inflation, SpringerBriefs in Physics, Springer (9, 2020), 10.1007/978-3-030-56810-8

    K. Lozanov,Reheating After Inflation, SpringerBriefs in Physics, Springer (9, 2020), 10.1007/978-3-030-56810-8

  37. [37]

    Barman, N

    B. Barman, N. Bernal and J. Rubio,Two or three things particle physicists (mis)understand about (pre)heating,Nucl. Phys. B1018(2025) 116996 [2503.19980]

  38. [38]

    Allahverdi et al.,The First Three Seconds: a Review of Possible Expansion Histories of the Early Universe,Open J

    R. Allahverdi et al.,The First Three Seconds: a Review of Possible Expansion Histories of the Early Universe,Open J. Astrophys.4(2021) astro.2006.16182 [2006.16182]

  39. [39]

    Batell et al.,Conversations and deliberations: Non-standard cosmological epochs and expansion histories,Int

    B. Batell et al.,Conversations and deliberations: Non-standard cosmological epochs and expansion histories,Int. J. Mod. Phys. A40(2025) 2530004 [2411.04780]

  40. [40]

    Bernal, K

    N. Bernal, K. Deka and M. Losada,Dark matter ultraviolet freeze-in in general reheating scenarios,Phys. Rev. D111(2025) 055034 [2501.04774]

  41. [41]

    Bernal, K

    N. Bernal, K. Deka and M. Losada,Thermal dark matter with low-temperature reheating, JCAP09(2024) 024 [2406.17039]

  42. [42]

    Bernal and Y

    N. Bernal and Y. Xu,Thermal gravitational waves during reheating,JHEP01(2025) 137 [2410.21385]

  43. [43]

    Bernal, C.S

    N. Bernal, C.S. Fong and ´O. Zapata,Probing low-reheating scenarios with minimal freeze-in dark matter,JHEP02(2025) 161 [2412.04550]

  44. [44]

    Banik, N

    A. Banik, N. Bernal and F. Hajkarim,Primordial Gravitational Waves from Phase Transitions during Reheating,2506.02116

  45. [45]

    Bernal, S

    N. Bernal, S. Mukherjee and J. Unwin,Boltzmann suppressed ultraviolet freeze-in,JCAP02 (2026) 010 [2510.01311]

  46. [46]

    Starobinsky,A New Type of Isotropic Cosmological Models Without Singularity,Phys

    A.A. Starobinsky,A New Type of Isotropic Cosmological Models Without Singularity,Phys. Lett. B91(1980) 99

  47. [47]

    Drees and Y

    M. Drees and Y. Xu,Small field polynomial inflation: reheating, radiative stability and lower bound,JCAP09(2021) 012 [2104.03977]

  48. [48]

    Bernal and Y

    N. Bernal and Y. Xu,Polynomial inflation and dark matter,Eur. Phys. J. C81(2021) 877 [2106.03950]

  49. [49]

    Drees and Y

    M. Drees and Y. Xu,Large field polynomial inflation: parameter space, predictions and (double) eternal nature,JCAP12(2022) 005 [2209.07545]

  50. [50]

    Bernal, J

    N. Bernal, J. Harz, M.A. Mojahed and Y. Xu,Graviton- and inflaton-mediated dark matter production after large field polynomial inflation,Phys. Rev. D111(2025) 043517 [2406.19447]

  51. [51]

    Kallosh and A

    R. Kallosh and A. Linde,Universality Class in Conformal Inflation,JCAP07(2013) 002 [1306.5220]

  52. [52]

    Kallosh and A

    R. Kallosh and A. Linde,Non-minimal Inflationary Attractors,JCAP10(2013) 033 [1307.7938]

  53. [53]

    R.T. Co, E. Gonz´ alez and K. Harigaya,Increasing Temperature toward the Completion of Reheating,JCAP11(2020) 038 [2007.04328]

  54. [54]

    Garc´ ıa, K

    M.A.G. Garc´ ıa, K. Kaneta, Y. Mambrini and K.A. Olive,Inflaton Oscillations and Post-Inflationary Reheating,JCAP04(2021) 012 [2012.10756]

  55. [55]

    Xu,Constraining axion and ALP dark matter from misalignment during reheating,Phys

    Y. Xu,Constraining axion and ALP dark matter from misalignment during reheating,Phys. Rev. D108(2023) 083536 [2308.15322]

  56. [56]

    Barman, N

    B. Barman, N. Bernal and Y. Xu,Resonant reheating,JCAP08(2024) 014 [2404.16090]. – 27 –

  57. [57]

    Barman, N

    B. Barman, N. Bernal, Y. Xu and ´O. Zapata,Ultraviolet freeze-in with a time-dependent inflaton decay,JCAP07(2022) 019 [2202.12906]

  58. [58]

    Chowdhury and A

    D. Chowdhury and A. Hait,Thermalization in the presence of a time-dependent dissipation and its impact on dark matter production,JHEP09(2023) 085 [2302.06654]

  59. [59]

    Cosme, F

    C. Cosme, F. Costa and O. Lebedev,Temperature evolution in the Early Universe and freeze-in at stronger coupling,JCAP06(2024) 031 [2402.04743]

  60. [60]

    B´ elanger, N

    G. B´ elanger, N. Bernal and A. Pukhov,Z’-mediated dark matter with low-temperature reheating,JHEP03(2025) 079 [2412.12303]

  61. [61]

    B´ elanger, N

    G. B´ elanger, N. Bernal and A. Pukhov,Strongly interacting singlet scalar dark matter during reheating,2603.05590

  62. [62]

    Winkler,Decay and detection of a light scalar boson mixing with the Higgs boson,Phys

    M.W. Winkler,Decay and detection of a light scalar boson mixing with the Higgs boson,Phys. Rev. D99(2019) 015018 [1809.01876]

  63. [63]

    Blackstone, J

    P.J. Blackstone, J. Tarr´ us Castell` a, E. Passemar and J. Zupan,Hadronic Decays of a Higgs-mixed Scalar,2407.13587

  64. [64]

    Blackstone.https://github.com/blackstonep/hipsofcobra, 2024

    P.J. Blackstone.https://github.com/blackstonep/hipsofcobra, 2024

  65. [65]

    B´ elanger, S

    G. B´ elanger, S. Chakraborti and A. Pukhov,Work in preparation, 2026. [66]LZcollaboration,First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment, Phys. Rev. Lett.131(2023) 041002 [2207.03764]. [67]LZcollaboration,Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment,Phys. Rev. Lett.135(2025) 011802 [2...

  66. [66]

    B´ elanger, A

    G. B´ elanger, A. Mjallal and A. Pukhov,Recasting direct detection limits within micrOMEGAs and implication for non-standard Dark Matter scenarios,Eur. Phys. J. C81(2021) 239 [2003.08621]

  67. [67]

    B´ elanger, F

    G. B´ elanger, F. Boudjema, P. Brun, A. Pukhov, S. Rosier-Lees, P. Salati et al.,Indirect search for dark matter with micrOMEGAs2.4,Comput. Phys. Commun.182(2011) 842 [1004.1092]. [70]Planckcollaboration,Planck 2018 results. VI. Cosmological parameters,Astron. Astrophys. 641(2020) A6 [1807.06209]

  68. [68]

    Slatyer,Indirect Dark Matter Signatures in the Cosmic Dark Ages II

    T.R. Slatyer,Indirect Dark Matter Signatures in the Cosmic Dark Ages II. Ionization, Heating and Photon Production from Arbitrary Energy Injections,Phys. Rev. D93(2016) 023521 [1506.03812]

  69. [69]

    Ciafaloni, D

    P. Ciafaloni, D. Comelli, A. Riotto, F. Sala, A. Strumia and A. Urbano,Weak Corrections are Relevant for Dark Matter Indirect Detection,JCAP03(2011) 019 [1009.0224]

  70. [70]

    Cirelli, G

    M. Cirelli, G. Corcella, A. Hektor, G. Hutsi, M. Kadastik, P. Panci et al.,PPPC 4 DM ID: A Poor Particle Physicist Cookbook for Dark Matter Indirect Detection,JCAP03(2011) 051 [1012.4515]

  71. [71]

    Calore, B

    F. Calore, B. Zald´ ıvar, P. Serpico and C. Eckner,Dark matter constraints from dwarf galaxies: a data-driven lat analysis, Oct., 2021. 10.5281/zenodo.5592836

  72. [72]

    B´ elanger, A

    G. B´ elanger, A. Mjallal and A. Pukhov,Two dark matter candidates: The case of inert doublet and singlet scalars,Phys. Rev. D105(2022) 035018 [2108.08061]

  73. [73]

    Arina, M

    C. Arina, M. Di Mauro, N. Fornengo, J. Heisig, A. Jueid and R.R. de Austri,CosmiXs: cosmic messenger spectra for indirect dark matter searches,JCAP03(2024) 035 [2312.01153]

  74. [74]

    Bierlich et al.,A comprehensive guide to the physics and usage of PYTHIA 8.3,SciPost Phys

    C. Bierlich et al.,A comprehensive guide to the physics and usage of PYTHIA 8.3,SciPost Phys. Codeb.2022(2022) 8 [2203.11601]

  75. [75]

    Altakach, S

    M.M. Altakach, S. Kraml, A. Lessa, S. Narasimha, T. Pascal, C. Ramos et al.,SModelS v3: going beyondZ 2 topologies,JHEP11(2024) 074 [2409.12942]. – 28 – [79]CMScollaboration,Search for resonant and nonresonant new phenomena in high-mass dilepton final states at √s= 13 TeV,JHEP07(2021) 208 [2103.02708]

  76. [76]

    Accomando, A

    E. Accomando, A. Belyaev, L. Fedeli, S.F. King and C. Shepherd-Themistocleous,Z’ physics with early LHC data,Phys. Rev. D83(2011) 075012 [1010.6058]

  77. [77]

    Amoroso, S

    S. Amoroso, S. Caron, A. Jueid, R. Ruiz de Austri and P. Skands,Estimating QCD uncertainties in Monte Carlo event generators for gamma-ray dark matter searches,JCAP05 (2019) 007 [1812.07424]

  78. [78]

    Jueid, J

    A. Jueid, J. Kip, R.R. de Austri and P. Skands,Impact of QCD uncertainties on antiproton spectra from dark-matter annihilation,JCAP04(2023) 068 [2202.11546]

  79. [79]

    Bonnivard et al.,Dark matter annihilation and decay in dwarf spheroidal galaxies: The classical and ultrafaint dSphs,Mon

    V. Bonnivard et al.,Dark matter annihilation and decay in dwarf spheroidal galaxies: The classical and ultrafaint dSphs,Mon. Not. Roy. Astron. Soc.453(2015) 849 [1504.02048]. [84]Fermi-LAT, DEScollaboration,Searching for Dark Matter Annihilation in Recently Discovered Milky Way Satellites with Fermi-LAT,Astrophys. J.834(2017) 110 [1611.03184]. [85]XENONco...

  80. [80]

    Baudis,DARWIN/XLZD: A future xenon observatory for dark matter and other rare interactions,Nucl

    L. Baudis,DARWIN/XLZD: A future xenon observatory for dark matter and other rare interactions,Nucl. Phys. B1003(2024) 116473 [2404.19524]

Showing first 80 references.