REVIEW 2 major objections 5 minor 74 references
Multipolar Dark Matter Freeze-out in an Early Matter-Dominated Universe
T0 review · 2 major / 5 minor · reviewed 2026-07-10 · grok-4.5
Pith's one-line read Early matter domination dilutes multipole dark matter, reopening parameter space that standard cosmology excludes.
desk verdict Solid incremental paper: entropy dilution reopens windows for three of four multipole operators under early matter domination, with clean analytics and honest flags on the approximations. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
Analytic matter-dominated freeze-out formulae (relic density and freeze-out temperature) that incorporate the entropy-dilution factor ζ arising from the sudden decay of a heavy field ϕ; these replace the standard radiation-dominated expressions and map each multipole operator onto a lower required coupling.
What would settle it
A complete numerical solution of the coupled Boltzmann equations that includes continuous ϕ decay during freeze-out, for the same multipole operators and the same reheating temperatures, would show whether the lower-coupling contours remain viable once entropy injection is treated continuously.
Extended reading notes
Core claim
Entropy dilution from an early matter-dominated era substantially lowers the multipole couplings needed to match the observed dark-matter relic density, thereby restoring viability to regions of magnetic-dipole, anapole and charge-radius parameter space that are excluded by direct detection and IceCube solar-neutrino bounds when freeze-out is assumed to occur in a radiation-dominated Universe.
Load-bearing premise
The calculation assumes freeze-out finishes while the Universe is still purely matter-dominated and entropy is conserved, before the heavy field begins to decay; if that hierarchy fails, the analytic formulae no longer apply.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies thermal freeze-out of fermionic dark matter that couples to the photon through dimension-5 and dimension-6 electromagnetic multipole operators (magnetic dipole, electric dipole, anapole, charge radius) in an early matter-dominated cosmology driven by a long-lived heavy field φ. Analytic solutions of the Boltzmann equation (App. A) yield the freeze-out abundance and the subsequent entropy-dilution factor ζ that relates it to the observed relic density (Eqs. 17–19). The required couplings are mapped in the (m_χ, g/Λ) or (m_χ, g/Λ^{2}) planes for several reheating temperatures and compared with radiation-dominated freeze-out and with current direct-detection and IceCube solar-neutrino limits. The central claim is that entropy dilution substantially lowers the interaction strength needed for Ωh^{2} = 0.12, reopening regions that are excluded under standard radiation domination, most notably for the anapole operator at low T_RH.
Significance. If the result holds, it shows that the pre-BBN expansion history is an essential ingredient in the phenomenology of electromagnetic multipole dark matter: regions that appear ruled out by direct detection and solar neutrinos under radiation domination become viable once entropy injection is taken into account. The work supplies explicit analytic formulae for the matter-dominated yield, carefully derived non-relativistic annihilation cross sections (App. B), and a transparent set of consistency conditions (Sec. II D) that mark where the pure-MD treatment is self-consistent. These ingredients make the qualitative conclusion falsifiable and useful for future model-building and experimental reinterpretation.
major comments (2)
- The analytic relic-density formulae (Eqs. 17–19) and the solid-black segments of the contours rest on the pure-MD, entropy-conserving, sudden-decay hierarchy T_f ≫ T_Γ, T_RH (Sec. II C, App. C). While the paper correctly greys out the T_f < T_Γ segments and states that a coupled evolution is then required, the quantitative size of the reopened windows for T_RH = 0.1 GeV and 10 GeV is still quoted from those formulae. A short numerical check (or an explicit statement of the residual uncertainty) for at least one benchmark point near the edge of the solid-black region would strengthen that the dilution factor remains accurate enough to support the claim that previously excluded parameter space is reopened.
- The analysis is restricted to m_χ < m_W to avoid the spurious high-energy growth of the W^{+}W^{-} channels (Sec. III B). This is a legitimate EFT cut, but it leaves the phenomenologically interesting multi-hundred-GeV to TeV window unexplored. Because the paper already flags the need for a full gauge-invariant basis including Z and Higgs operators, a brief estimate of how the relic contours would shift once those channels are restored (or an explicit deferral with a quantitative caveat) would clarify the scope of the “reopened” regions advertised in the abstract and Sec. IV.
minor comments (5)
- Abstract and Sec. IV: the phrase “confront it with current constraints” should be “confront them” (subject–verb agreement).
- Figs. 1 and 2: the solid-black versus grey distinction for T_f ≳ T_Γ is explained only in the caption; a short sentence in the main text of Sec. IV would help readers who look first at the figures.
- Table I (NR structures): the charge-radius entry lists the operator as χ̄ γ^μ γ^{5} χ J_μ, which appears to be a typographical mix-up with the anapole; the correct CR structure is the vector current without γ^{5}.
- Eq. (16) for g_eff^{1/2}: the approximation used later in App. A (g_eff^{1/2} ≃ (3/4) g_igstar^{1/2} (1−r)^{-½} x^{-½} x_igstar^{1/2}) is stated only after the fact; a forward reference would improve readability.
- Note Added: the arXiv number of the concurrent work is given as 2607.01390; a quick consistency check of the citation would avoid a possible typographical error.
Circularity Check
No significant circularity: relic contours are computed from free cosmological parameters and external Ωh², then compared to independent experimental bounds.
full rationale
The paper's central claim is that entropy dilution from early matter domination lowers the multipole couplings needed for Ωχh² = 0.12, reopening regions excluded under radiation-dominated freeze-out. The derivation chain is: (i) free parameters T⋆, r, TRH define the modified Hubble and dilution factor ζ (Eqs. 1–9, 7); (ii) multipole operators yield ⟨σv⟩ expansions (Sec. III A, App. B) that are standard EFT results; (iii) the Boltzmann equation is solved analytically under the pure-MD, sudden-decay assumptions (App. A, Eqs. 17–19) to obtain the coupling that matches the external Planck benchmark Ωh² = 0.12; (iv) the resulting contours are overlaid on external direct-detection and IceCube limits. None of these steps is self-definitional, a fitted input re-used as a prediction, or a uniqueness claim imported from the authors' prior work. Self-citations supply cross-sections or earlier multipole phenomenology but are not load-bearing for the dilution effect itself. The sudden-decay hierarchy is an explicit assumption whose breakdown is marked (gray contour segments) rather than hidden. The result is therefore a genuine parameter-space comparison, not a circular construction.
Assumptions & free parameters
free parameters (4)
- T_⋆ =
10^5 GeV
- r =
0.99
- T_RH =
0.1, 10, 10^3 GeV
- g/Λ or g/Λ²
assumptions (5)
- domain assumption Universe undergoes an early matter-dominated era driven by a long-lived heavy field ϕ that later decays and injects entropy before BBN.
- domain assumption Sudden-decay approximation: entropy is conserved until ϕ decays instantaneously at T_Γ ≈ T_RH.
- ad hoc to paper Only one multipole operator is present at a time; all other coefficients are set to zero.
- domain assumption EFT description restricted to m_χ < m_W so that photon-only operators remain gauge-invariant and free of spurious energy growth.
- standard math Standard thermal freeze-out Boltzmann equation with NR velocity expansion of ⟨σv⟩.
invented entities (1)
-
long-lived heavy field ϕ
Cite this review
Pith. "Pith review of Multipolar Dark Matter Freeze-out in an Early Matter-Dominated Universe." pith.science (2026). https://pith.science/paper/CKBSRRTX
@misc{pith2026260707956,
author = {Pith},
title = {Pith review of: Multipolar Dark Matter Freeze-out in an Early Matter-Dominated Universe},
year = {2026},
howpublished = {\url{https://pith.science/paper/CKBSRRTX}},
note = {Machine review of arXiv:2607.07956}
}
read the original abstract
The relic abundance of thermal dark matter depends not only on its particle interactions but also on the expansion history of the early Universe. We study the freeze-out of fermionic dark matter interacting with the Standard Model through higher-dimensional electromagnetic operators in an early matter-dominated cosmology. In particular, we consider magnetic dipole, electric dipole, anapole, and charge-radius interactions, and compute the couplings required to reproduce the observed dark matter relic abundance in the presence of entropy injection from the decay of a long-lived heavy field. The resulting parameter space is compared with that obtained in the standard radiation-dominated freeze-out scenario and confront it with current constraints from direct-detection experiments and solar neutrino observations. We find that the entropy dilution associated with an early matter-dominated epoch significantly reduces the interaction strength required to obtain the observed relic abundance, thereby rendering viable regions of parameter space that are excluded in the conventional cosmological history. Our results demonstrate that the cosmological history prior to Big Bang nucleosynthesis can have an important impact on the phenomenology and experimental viability of electromagnetic multipole dark matter.
Figures
Reference graph
Works this paper leans on
-
[1]
Calculation for the freeze-out temperature At freeze-out the DM relic abundance stop tracking the equilibrium abundance, hence, ∆χ(xf)≃Y χ,eq(xf) =δ χYχ,eq(xf), (A9) whereδ χ is a order of unity factor. Neglectingd∆ χ/dxnear freeze-out, from Eq. (A2) we may write dYχ dx f ≈ − X n λn δχ(δχ + 2)x −n−2 f g1/2 eff (xf)Y 2 χ,eq(xf). (A10) Also, dYχ,eq dx =Y χ,...
-
[2]
The First Three Seconds: a Review of Possible Expansion Histories of the Early Universe
R. Allahverdiet al., The First Three Seconds: a Re- view of Possible Expansion Histories of the Early Uni- verse, Open J. Astrophys.4, astro.2006.16182 (2021), arXiv:2006.16182 [astro-ph.CO]
work page Pith review arXiv 2006
-
[3]
M. Kamionkowski and M. S. Turner, Thermal Relics: Do We Know Their Abundances?, Phys. Rev. D42, 3310 (1990)
work page 1990
- [4]
-
[5]
Wino Cold Dark Matter from Anomaly-Mediated SUSY Breaking
T. Moroi and L. Randall, Wino cold dark matter from anomaly mediated SUSY breaking, Nucl. Phys. B570, 455 (2000), arXiv:hep-ph/9906527
work page Pith review arXiv 2000
- [6]
-
[7]
The effect of a late decaying scalar on the neutralino relic density
G. Gelmini, P. Gondolo, A. Soldatenko, and C. E. Ya- guna, The Effect of a late decaying scalar on the neu- tralino relic density, Phys. Rev. D74, 083514 (2006), arXiv:hep-ph/0605016
work page Pith review arXiv 2006
-
[8]
G. B. Gelmini and P. Gondolo, Neutralino with the right cold dark matter abundance in (almost) any su- persymmetric model, Phys. Rev. D74, 023510 (2006), arXiv:hep-ph/0602230
work page Pith review arXiv 2006
Show all 74 references
-
[9]
B. S. Acharya, G. Kane, S. Watson, and P. Kumar, A Non-thermal WIMP Miracle, Phys. Rev. D80, 083529 (2009), arXiv:0908.2430 [astro-ph.CO]
2009 arXiv
-
[10]
G. L. Kane, P. Kumar, B. D. Nelson, and B. Zheng, Dark matter production mechanisms with a nonthermal cosmological history: A classification, Phys. Rev. D93, 063527 (2016), arXiv:1502.05406 [hep-ph]
2016 arXiv
-
[11]
Davoudiasl, D
H. Davoudiasl, D. Hooper, and S. D. McDermott, Inflat- able Dark Matter, Phys. Rev. Lett.116, 031303 (2016), arXiv:1507.08660 [hep-ph]
2016 arXiv
-
[12]
Randall, J
L. Randall, J. Scholtz, and J. Unwin, Flooded Dark Mat- ter and S Level Rise, JHEP03, 011, arXiv:1509.08477 [hep-ph]
-
[13]
R. T. Co, F. D’Eramo, L. J. Hall, and D. Pappadop- ulo, Freeze-In Dark Matter with Displaced Signatures at Colliders, JCAP12, 024, arXiv:1506.07532 [hep-ph]
-
[14]
J. A. Dror, E. Kuflik, and W. H. Ng, Codecaying Dark Matter, Phys. Rev. Lett.117, 211801 (2016), arXiv:1607.03110 [hep-ph]
2016 arXiv
-
[15]
Banerjee and D
A. Banerjee and D. Chowdhury, Fingerprints of freeze-in dark matter in an early matter-dominated era, SciPost Phys.13, 022 (2022), arXiv:2204.03670 [hep-ph]
2022 arXiv
-
[16]
E. W. Kolb and M. S. Turner,The Early Universe, Vol. 69 (Taylor and Francis, 2019)
2019
-
[17]
Hamdan and J
S. Hamdan and J. Unwin, Dark Matter Freeze-out Dur- ing Matter Domination, Mod. Phys. Lett. A33, 1850181 (2018), arXiv:1710.03758 [hep-ph]
2018
-
[18]
Chanda, S
P. Chanda, S. Hamdan, and J. Unwin, RevivingZand Higgs Mediated Dark Matter Models in Matter Domi- nated Freeze-out, JCAP01, 034, arXiv:1911.02616 [hep- ph]
1911
-
[19]
Chanda and J
P. Chanda and J. Unwin, Decoupling of asymmetric dark matter during an early matter dominated era, JCAP06, 032, arXiv:2102.02313 [hep-ph]
-
[20]
Steigman and M
G. Steigman and M. S. Turner, Cosmological Constraints on the Properties of Weakly Interacting Massive Parti- cles, Nucl. Phys. B253, 375 (1985)
1985
-
[21]
Jungman, M
G. Jungman, M. Kamionkowski, and K. Griest, Super- symmetric dark matter, Phys. Rept.267, 195 (1996), arXiv:hep-ph/9506380
1996 arXiv
-
[22]
Bertone, D
G. Bertone, D. Hooper, and J. Silk, Particle dark matter: Evidence, candidates and constraints, Phys. Rept.405, 279 (2005), arXiv:hep-ph/0404175
2005 arXiv
-
[23]
Steigman, B
G. Steigman, B. Dasgupta, and J. F. Beacom, Precise Relic WIMP Abundance and its Impact on Searches for Dark Matter Annihilation, Phys. Rev. D86, 023506 (2012), arXiv:1204.3622 [hep-ph]
2012 arXiv
-
[24]
Arcadi, M
G. Arcadi, M. Dutra, P. Ghosh, M. Lindner, Y. Mam- brini, M. Pierre, S. Profumo, and F. S. Queiroz, The waning of the WIMP? A review of models, searches, and constraints, Eur. Phys. J. C78, 203 (2018), arXiv:1703.07364 [hep-ph]
2018 arXiv
-
[25]
W. L. Xu, C. Dvorkin, and A. Chael, Probing sub- GeV Dark Matter-Baryon Scattering with Cosmolog- ical Observables, Phys. Rev. D97, 103530 (2018), arXiv:1802.06788 [astro-ph.CO]
2018 arXiv
-
[26]
Dvorkin, T
C. Dvorkin, T. Lin, and K. Schutz, Making dark matter out of light: freeze-in from plasma effects, Phys. Rev. D 99, 115009 (2019), [Erratum: Phys.Rev.D 105, 119901 (2022)], arXiv:1902.08623 [hep-ph]
2019 arXiv
-
[27]
J. H. Chang, R. Essig, and S. D. McDermott, Super- nova 1987A Constraints on Sub-GeV Dark Sectors, Mil- licharged Particles, the QCD Axion, and an Axion-like Particle, JHEP09, 051, arXiv:1803.00993 [hep-ph]
-
[28]
Caputo, L
A. Caputo, L. Sberna, M. Frias, D. Blas, P. Pani, L. Shao, and W. Yan, Constraints on millicharged dark matter and axionlike particles from timing of radio waves, Phys. Rev. D100, 063515 (2019), arXiv:1902.02695 [astro- ph.CO]
2019 arXiv
-
[29]
E. Iles, S. Heeba, and K. Schutz, Dark Matter Di- rect Detection Experiments Are Sensitive to the Mil- licharged Background, Phys. Rev. Lett.134, 121002 (2025), arXiv:2407.21096 [hep-ph]
2025 arXiv
-
[30]
I. B. Zel’dovich, Electromagnetic Interaction with Parity Violation, Sov. Phys. JETP6, 1184 (1958)
1958
-
[31]
Pospelov and T
M. Pospelov and T. ter Veldhuis, Direct and indirect lim- its on the electromagnetic form-factors of WIMPs, Phys. Lett. B480, 181 (2000), arXiv:hep-ph/0003010
2000 arXiv
-
[32]
Sigurdson, M
K. Sigurdson, M. Doran, A. Kurylov, R. R. Caldwell, and M. Kamionkowski, Dark-matter electric and mag- netic dipole moments, Phys. Rev. D70, 083501 (2004), [Erratum: Phys.Rev.D 73, 089903 (2006)], arXiv:astro- ph/0406355
2004
-
[33]
Masso, S
E. Masso, S. Mohanty, and S. Rao, Dipolar Dark Matter, Phys. Rev. D80, 036009 (2009), arXiv:0906.1979 [hep- ph]
2009 arXiv
-
[34]
Barger, W.-Y
V. Barger, W.-Y. Keung, and D. Marfatia, Electro- magnetic properties of dark matter: Dipole moments and charge form factor, Phys. Lett. B696, 74 (2011), arXiv:1007.4345 [hep-ph]
2011 arXiv
-
[35]
C. M. Ho and R. J. Scherrer, Anapole Dark Matter, Phys. Lett. B722, 341 (2013), arXiv:1211.0503 [hep-ph]
2013 arXiv
-
[36]
B. J. Kavanagh, P. Panci, and R. Ziegler, Faint Light from Dark Matter: Classifying and Constraining Dark Matter-Photon Effective Operators, JHEP04, 089, arXiv:1810.00033 [hep-ph]
-
[37]
Hambye and X.-J
T. Hambye and X.-J. Xu, Dark matter electromag- 16 netic dipoles: the WIMP expectation, JHEP11, 156, arXiv:2106.01403 [hep-ph]
-
[38]
Ibarra, M
A. Ibarra, M. Reichard, and R. Nagai, Anapole mo- ment of Majorana fermions and implications for direct detection of neutralino dark matter, JHEP01, 086, arXiv:2207.01014 [hep-ph]
-
[39]
E. E. Radescu, On the Electromagnetic Properties of Ma- jorana Fermions, Phys. Rev. D32, 1266 (1985)
1985
-
[40]
Banks, J.-F
T. Banks, J.-F. Fortin, and S. Thomas, Direct Detec- tion of Dark Matter Electromagnetic Dipole Moments, (2010), arXiv:1007.5515 [hep-ph]
2010 arXiv
-
[41]
Del Nobile, G
E. Del Nobile, G. B. Gelmini, P. Gondolo, and J.-H. Huh, Direct detection of Light Anapole and Magnetic Dipole DM, JCAP06, 002, arXiv:1401.4508 [hep-ph]
-
[42]
D. Bose, D. Chowdhury, P. Mondal, and T. S. Ray, Trou- bles mounting for multipolar dark matter, JHEP06, 014, arXiv:2312.05131 [hep-ph]
-
[43]
Ibarra, M
A. Ibarra, M. Reichard, and G. Tomar, Probing dark matter electromagnetic properties in direct detection ex- periments, JCAP02, 072, arXiv:2408.15760 [hep-ph]
-
[44]
Kumar, B
J. Kumar, B. Mondal, G. Muralidhara, and N. Raj, Di- rect detection of electromagnetically interacting ultra- heavy dark matter, (2025), arXiv:2509.24938 [hep-ph]
2025
-
[45]
Geytenbeek, S
B. Geytenbeek, S. Rao, P. Scott, A. Serenelli, A. C. Vin- cent, M. White, and A. G. Williams, Effect of electro- magnetic dipole dark matter on energy transport in the solar interior, JCAP03, 029, arXiv:1610.06737 [hep-ph]
-
[46]
Lambiase, S
G. Lambiase, S. Mohanty, A. Nautiyal, and S. Rao, Constraints on electromagnetic form factors of sub- GeV dark matter from the cosmic microwave back- ground anisotropy, Phys. Rev. D104, 023519 (2021), arXiv:2102.04840 [hep-ph]
2021 arXiv
-
[47]
Fortin and T
J.-F. Fortin and T. M. P. Tait, Collider Constraints on Dipole-Interacting Dark Matter, Phys. Rev. D85, 063506 (2012), arXiv:1103.3289 [hep-ph]
2012 arXiv
-
[48]
X. Chu, J. Pradler, and L. Semmelrock, Light dark states with electromagnetic form factors, Phys. Rev. D99, 015040 (2019), arXiv:1811.04095 [hep-ph]
2019 arXiv
-
[49]
R. J. Scherrer and M. S. Turner, Decaying particles do not “heat up” the Universe, Phys. Rev. D31, 681 (1985)
1985
-
[50]
Spokoiny, Deflationary universe scenario, Phys
B. Spokoiny, Deflationary universe scenario, Phys. Lett. B315, 40 (1993), arXiv:gr-qc/9306008
1993 arXiv
-
[51]
M. L. Graesser, I. M. Shoemaker, and L. Vec- chi, Asymmetric WIMP dark matter, JHEP10, 110, arXiv:1103.2771 [hep-ph]
-
[52]
R. J. Scherrer and M. S. Turner, On the Relic, Cos- mic Abundance of Stable Weakly Interacting Massive Particles, Phys. Rev. D33, 1585 (1986), [Erratum: Phys.Rev.D 34, 3263 (1986)]
1986
-
[53]
Del Nobile, The Theory of Direct Dark Matter De- tection: A Guide to Computations 10.1007/978-3-030- 95228-0 (2021), arXiv:2104.12785 [hep-ph]
E. Del Nobile, The Theory of Direct Dark Matter De- tection: A Guide to Computations 10.1007/978-3-030- 95228-0 (2021), arXiv:2104.12785 [hep-ph]
-
[54]
Y. Gao, C. M. Ho, and R. J. Scherrer, Anapole Dark Matter at the LHC, Phys. Rev. D89, 045006 (2014), arXiv:1311.5630 [hep-ph]
2014 arXiv
-
[55]
Arina, A
C. Arina, A. Cheek, K. Mimasu, and L. Pagani, Light and Darkness: consistently coupling dark matter to photons via effective operators, Eur. Phys. J. C81, 223 (2021), arXiv:2005.12789 [hep-ph]
2021 arXiv
-
[56]
S. Y. Choi, J. Jeong, D. W. Kang, and S. Shin, Hunting for hypercharge anapole dark matter in all spin scenarios, Phys. Rev. D109, 096001 (2024), arXiv:2401.02855 [hep- ph]
2024 arXiv
-
[57]
PandaX Collaboration, Limits on the luminance of dark matter from xenon recoil data, Nature618, 47 (2023)
2023
-
[58]
Liang, Y
J.-H. Liang, Y. Liao, X.-D. Ma, and H.-L. Wang, A systematic investigation on dark matter-electron scattering in effective field theories, JHEP07, 279, arXiv:2406.10912 [hep-ph]
-
[59]
Garani and S
R. Garani and S. Palomares-Ruiz, Dark matter in the Sun: scattering off electrons vs nucleons, JCAP05, 007, arXiv:1702.02768 [hep-ph]
-
[60]
Busoni, A
G. Busoni, A. De Simone, P. Scott, and A. C. Vin- cent, Evaporation and scattering of momentum- and velocity-dependent dark matter in the Sun, JCAP10, 037, arXiv:1703.07784 [hep-ph]
-
[61]
Bose and S
D. Bose and S. Sarkar, Impact of galactic distributions in celestial capture of dark matter, Phys. Rev. D107, 063010 (2023), arXiv:2211.16982 [astro-ph.CO]
2023 arXiv
-
[62]
Vinyoles, A
N. Vinyoles, A. M. Serenelli, F. L. Villante, S. Basu, J. Bergstr¨ om, M. C. Gonzalez-Garcia, M. Maltoni, C. Pe˜ na-Garay, and N. Song, A new Generation of Standard Solar Models, Astrophys. J.835, 202 (2017), arXiv:1611.09867 [astro-ph.SR]
2017 arXiv
-
[63]
R. H. Helm, Inelastic and Elastic Scattering of 187-Mev Electrons from Selected Even-Even Nuclei, Phys. Rev. 104, 1466 (1956)
1956
-
[64]
Liang, Y.-L
Z.-L. Liang, Y.-L. Tang, and Z.-Q. Yang, The leptophilic dark matter in the Sun: the minimum testable mass, JCAP10, 035, arXiv:1802.01005 [hep-ph]
-
[65]
Garani and S
R. Garani and S. Palomares-Ruiz, Evaporation of dark matter from celestial bodies, JCAP05(05), 042, arXiv:2104.12757 [hep-ph]
-
[66]
Q. Liu, J. Lazar, C. A. Arg¨ uelles, and A. Kheirandish, χaroν: a tool for neutrino flux generation from WIMPs, JCAP10, 043, arXiv:2007.15010 [hep-ph]
2007 arXiv
-
[67]
C. A. Arg¨ uelles, J. Salvado, and C. N. Weaver, nuSQuIDS: A toolbox for neutrino propagation, Comput. Phys. Commun.277, 108346 (2022), arXiv:2112.13804 [hep-ph]
2022 arXiv
-
[68]
T. N. Maity, A. K. Saha, S. Mondal, and R. Laha, Neutrinos from the Sun can discover dark matter- electron scattering, Phys. Rev. D112, 023025 (2025), arXiv:2308.12336 [hep-ph]
2025 arXiv
-
[69]
M. G. Aartsenet al.(IceCube), Search for annihilating dark matter in the Sun with 3 years of IceCube data, Eur. Phys. J. C77, 146 (2017), [Erratum: Eur.Phys.J.C 79, 214 (2019)], arXiv:1612.05949 [astro-ph.HE]
2017 arXiv
-
[70]
Abbasiet al.(IceCube), Search for GeV-scale dark matter annihilation in the Sun with IceCube DeepCore, Phys
R. Abbasiet al.(IceCube), Search for GeV-scale dark matter annihilation in the Sun with IceCube DeepCore, Phys. Rev. D105, 062004 (2022), arXiv:2111.09970 [astro-ph.HE]
2022
-
[71]
Aghanimet al.(Planck), Planck 2018 results
N. Aghanimet al.(Planck), Planck 2018 results. VI. Cosmological parameters, Astron. Astrophys.641, A6 (2020), [Erratum: Astron.Astrophys. 652, C4 (2021)], arXiv:1807.06209 [astro-ph.CO]
2018 arXiv
-
[72]
Anand, A
N. Anand, A. L. Fitzpatrick, and W. C. Haxton, Weakly interacting massive particle-nucleus elastic scattering re- sponse, Phys. Rev. C89, 065501 (2014), arXiv:1308.6288 [hep-ph]
2014 arXiv
-
[73]
J. C. Criado, A. Djouadi, M. Perez-Victoria, and J. San- tiago, A complete effective field theory for dark matter, JHEP07, 081, arXiv:2104.14443 [hep-ph]
-
[74]
Jahedi, Neutron stars as thermometers for reheating induced dipole dark matter, (2026), arXiv:2607.01390 [hep-ph]
S. Jahedi, Neutron stars as thermometers for reheating induced dipole dark matter, (2026), arXiv:2607.01390 [hep-ph]
2026 arXiv
Reviewed July 10, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.