REVIEW 2 major objections 41 references
Constraints on the Injection of Radiation in the Early Universe
T0 review · 2 major / 0 minor · reviewed 2026-05-10 · grok-4.3
Pith's one-line read Injecting mixed dark and electromagnetic radiation after BBN but before recombination is constrained to no more than about 25 percent more total extra radiation than the pure dark radiation case.
desk verdict Mixed radiation injection only relaxes the bound by 25% due to baryon dilution, with the numerical study needing more scrutiny. 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
Dilution of the baryon-to-entropy ratio by electromagnetic radiation, which supplies an independent constraint beyond the net effect on the effective number of neutrinos.
What would settle it
An observation of Neff or the baryon-to-entropy ratio at recombination that permits more than 25% extra radiation while remaining consistent with BBN data without dilution.
Extended reading notes
Core claim
When radiation is injected generically during the epoch between BBN and recombination, the opposite-sign contributions of dark and electromagnetic components to the effective neutrino number are offset by the dilution of the baryon-to-entropy ratio caused by the electromagnetic part. This dilution must remain consistent with the ratio inferred from both BBN and recombination observations. Numerical studies demonstrate that the allowed total extra radiation is at most ∼25% greater than the amount permitted under the assumption of purely dark radiation.
Load-bearing premise
Electromagnetic radiation injection dilutes the baryon-to-entropy ratio in a manner that must match independent measurements at both BBN and recombination without other compensating effects.
Editorial extensions
If this is right
- Models that inject radiation after BBN must satisfy both the Neff bound and the baryon dilution bound simultaneously.
- Purely electromagnetic radiation injection would face even tighter limits than the mixed case.
- Precision cosmology measurements of Neff and the baryon density at multiple epochs can directly test such injection scenarios.
- The result restricts the parameter space for new physics that produces radiation in this epoch.
Reading between the lines
- Distinguishing dark from electromagnetic injection may require observables other than Neff alone.
- The bound could be applied to constrain late-decaying particles or other sources that produce mixed radiation.
- Similar dilution effects might appear in related early-universe processes involving entropy changes.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript examines the injection of both dark radiation and electromagnetic radiation between BBN and recombination. Although the two components contribute with opposite signs to the effective number of relativistic species, electromagnetic injection increases entropy and thereby dilutes the baryon-to-entropy ratio η, which is independently measured at BBN and at recombination. A numerical study is reported to show that the total allowed extra radiation cannot exceed the pure-dark-radiation limit by more than ∼25%.
Significance. If the numerical bound is robust, the result supplies a concrete, observationally anchored limit on mixed radiation injection that is tighter than the pure-dark-radiation case alone. It underscores the diagnostic power of the η consistency window and could be used to sharpen constraints on early-universe extensions that produce both dark and electromagnetic energy.
major comments (2)
- [Abstract] Abstract: the central quantitative claim that extra radiation is allowed to be no more than ∼25% above the pure-dark-radiation limit rests on an unspecified numerical study; no information is given on the simulation setup, input parameters, data sets (BBN or CMB likelihoods), error propagation, or validation against known limits, preventing assessment of the result's reliability.
- [Abstract] The dilution argument implicitly assumes that no other early-universe degree of freedom (post-BBN expansion-rate shift, small variation in baryon loading, or recombination-history change) can partially compensate the entropy increase and thereby permit a larger electromagnetic component while still satisfying both η measurements; no explicit marginalization or degeneracy test is described.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for identifying areas where additional clarity would strengthen the presentation. We address each major comment below and have made revisions to improve transparency and acknowledge limitations.
read point-by-point responses
-
Referee: [Abstract] Abstract: the central quantitative claim that extra radiation is allowed to be no more than ∼25% above the pure-dark-radiation limit rests on an unspecified numerical study; no information is given on the simulation setup, input parameters, data sets (BBN or CMB likelihoods), error propagation, or validation against known limits, preventing assessment of the result's reliability.
Authors: The numerical study is described in Sections 3 and 4 of the manuscript, which detail the modeling of sudden radiation injection, the adjustment of the baryon-to-photon ratio for entropy dilution using standard BBN calculations, and the application of Planck CMB likelihoods at recombination. A grid-based scan over injection parameters with validation against the pure dark-radiation case is employed. To make this information accessible without requiring the reader to consult the body text, we have revised the abstract to include a concise summary of the methodology, data sets, and validation procedure. revision: yes
-
Referee: [Abstract] The dilution argument implicitly assumes that no other early-universe degree of freedom (post-BBN expansion-rate shift, small variation in baryon loading, or recombination-history change) can partially compensate the entropy increase and thereby permit a larger electromagnetic component while still satisfying both η measurements; no explicit marginalization or degeneracy test is described.
Authors: We agree that the analysis isolates the entropy-dilution effect on η consistency and does not include a full marginalization over additional degrees of freedom that could partially compensate the dilution. This choice was made to focus on the primary mechanism under consideration. In the revised manuscript we have added an explicit statement in the discussion section acknowledging this assumption, noting that a broader degeneracy analysis lies beyond the present scope, and explaining why the η-dilution constraint is expected to remain dominant. revision: partial
Circularity Check
No significant circularity; constraints derived from external η measurements
full rationale
The paper's central result is a numerical study finding that extra radiation (dark + EM) is allowed at most ~25% above the pure-dark-radiation case. This bound follows from requiring consistency between the diluted baryon-to-entropy ratio after EM injection and the independently measured η values at BBN and recombination. No equations or steps reduce by construction to self-fitted parameters, self-citations, or ansatze; the derivation compares model outputs to external data without renormalization or uniqueness theorems imported from the authors' prior work. This is a standard, self-contained constraint analysis.
Assumptions & free parameters
assumptions (1)
- domain assumption Standard big bang nucleosynthesis and recombination physics apply without additional compensating effects
Cite this review
Pith. "Pith review of Constraints on the Injection of Radiation in the Early Universe." pith.science (2026). https://pith.science/paper/2604.05282
@misc{pith2026260405282,
author = {Pith},
title = {Pith review of: Constraints on the Injection of Radiation in the Early Universe},
year = {2026},
howpublished = {\url{https://pith.science/paper/2604.05282}},
note = {Machine review of arXiv:2604.05282}
}
abstract
We consider the generic injection of radiation (both dark and electromagnetic) during the epoch between big bang nucleosynthesis (BBN) and recombination. The contribution of the additional radiation to the number of effective neutrinos may be quite small in this scenario, since dark radiation and electromagnetic radiation provide contributions of opposite sign. However, the injection of electromagnetic radiation dilutes the baryon-to-entropy ratio, which is measured both at BBN and at recombination. As a result, this scenario is expected to be tightly constrained. Indeed, performing a numerical study, we find that the allowed amount of extra radiation may be no more than $\sim 25\%$ greater than in the case where it is assumed to be entirely dark radiation.
Figures
Figures from the paper (4 more)
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
performing a numerical study, we find that the allowed amount of extra radiation may be no more than ∼25% greater than in the case where it is assumed to be entirely dark radiation
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
the injection of electromagnetic radiation dilutes the baryon-to-entropy ratio
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
CMB Anisotropy Constraints Our analysis incorporates temperature and polariza- tion anisotropy measurements from thePlanck2018 data release [39]. We utilize the full likelihood pipeline con- sisting of three distinct components: high multipole cov- erage through the Plik TTTEEE likelihood spanning 30≤ℓ≤2508, complemented by the Commander tem- perature lik...
-
[2]
BBN Observable Constraints Our BBN likelihood construction relies on observed primordial abundances of light elements produced during the nucleosynthesis epoch. We incorporate two principal observables that provide complementary constraints on early universe cosmology: the primordial 4He mass frac- tion and the deuterium-to-hydrogen number ratio. Theo- re...
work page 1949
-
[3]
Novel two component dark matter features in the Z2 × Z2 3HDM
N. Aghanimet al.[Planck], “Planck 2018 re- sults. VI. Cosmological parameters,” Astron. Astro- phys.641, A6 (2020) [erratum: Astron. Astro- 9 phys.652, C4 (2021)] doi:10.1051/0004-6361/201833910 [arXiv:1807.06209 [astro-ph.CO]]
work page Pith review arXiv doi:10.1051/0004-6361/201833910 2018
-
[4]
S. Goldstein and J. C. Hill, “A 2% determination ofN eff from primordial element abundance, cosmic microwave background, and baryon acoustic oscillation measure- ments,” [arXiv:2603.13226 [astro-ph.CO]]
-
[5]
The Simons Observatory: science goals and forecasts
P. Adeet al.[Simons Observatory], “The Simons Observatory: Science goals and forecasts,” JCAP 02, 056 (2019) doi:10.1088/1475-7516/2019/02/056 [arXiv:1808.07445 [astro-ph.CO]]
-
[6]
M. Escudero, M. Ovchynnikov and N. Weiner, “What does it take to haveN eff <3 at CMB times?,” [arXiv:2603.22391 [hep-ph]]
-
[7]
F. Niedermann and M. S. Sloth, Phys. Rev. D103, no.4, L041303 (2021) doi:10.1103/PhysRevD.103.L041303 [arXiv:1910.10739 [astro-ph.CO]]
-
[8]
F. Niedermann and M. S. Sloth, Phys. Rev. D102, no.6, 063527 (2020) doi:10.1103/PhysRevD.102.063527 [arXiv:2006.06686 [astro-ph.CO]]
Show all 41 references
-
[9]
Hot new early dark energy bridging cosmic gaps: Supercooled phase transition reconciles stepped dark radiation solutions to the Hubble tension with BBN,
M. Garny, F. Niedermann, H. Rubira and M. S. Sloth, “Hot new early dark energy bridging cosmic gaps: Supercooled phase transition reconciles stepped dark radiation solutions to the Hubble tension with BBN,” Phys. Rev. D110, no.2, 023531 (2024) doi:10.1103/PhysRevD.110.023531 [...
2024 doi
-
[10]
Cos- mological and Astrophysical Constraints on Late First- Order Phase Transitions,
K. Greene, D. W. R. Ho, S. Kumar and Y. Tsai, “Cos- mological and Astrophysical Constraints on Late First- Order Phase Transitions,” [arXiv:2603.00272 [hep-ph]]
-
[11]
Bai and M
Y. Bai and M. Korwar, Phys. Rev. D105, no.9, 095015 (2022) doi:10.1103/PhysRevD.105.095015 [arXiv:2109.14765 [hep-ph]]
2022 doi
-
[12]
Bringmann, P
T. Bringmann, P. F. Depta, T. Konstandin, K. Schmidt- Hoberg and C. Tasillo, JCAP11, 053 (2023) doi:10.1088/1475-7516/2023/11/053 [arXiv:2306.09411 [astro-ph.CO]]
2023 doi
-
[13]
Was entropy conserved between BBN and recom- bination?,
A. C. Sobotka, A. L. Erickcek and T. L. Smith, “Was entropy conserved between BBN and recom- bination?,” Phys. Rev. D107, no.2, 023525 (2023) doi:10.1103/PhysRevD.107.023525 [arXiv:2207.14308 [astro-ph.CO]]
2023 doi
-
[14]
New Bounds for Axions and Axion-Like Particles with keV-GeV Masses,
M. Millea, L. Knox and B. Fields, “New Bounds for Axions and Axion-Like Particles with keV-GeV Masses,” Phys. Rev. D92, no.2, 023010 (2015) doi:10.1103/PhysRevD.92.023010 [arXiv:1501.04097 [astro-ph.CO]]
2015 doi
-
[16]
Cosmological bounds on pseudo Nambu-Goldstone bosons,
D. Cadamuro and J. Redondo, “Cosmological bounds on pseudo Nambu-Goldstone bosons,” JCAP02, 032 (2012) doi:10.1088/1475-7516/2012/02/032 [arXiv:1110.2895 [hep-ph]]
2012 doi
-
[18]
On a light spinless par- ticle coupled to photons,
E. Masso and R. Toldra, “On a light spinless par- ticle coupled to photons,” Phys. Rev. D52, 1755- 1763 (1995) doi:10.1103/PhysRevD.52.1755 [arXiv:hep- ph/9503293 [hep-ph]]
1995 doi
-
[20]
Joint Cosmic Microwave Background and Big Bang Nucleosynthesis Constraints on Light Dark Sectors with Dark Radiation,
C. Giovanetti, M. Lisanti, H. Liu and J. T. Ruderman, “Joint Cosmic Microwave Background and Big Bang Nucleosynthesis Constraints on Light Dark Sectors with Dark Radiation,” Phys. Rev. Lett.129, no.2, 021302 (2022) doi:10.1103/PhysRevLett.129.021302 [arXiv:2109.03246 [hep-ph]]
2022 doi
-
[22]
A Precision calculation of the effective number of cosmological neutrinos,
G. Mangano, G. Miele, S. Pastor and M. Peloso, “A Precision calculation of the effective number of cosmological neutrinos,” Phys. Lett. B534, 8-16 (2002) doi:10.1016/S0370-2693(02)01622-2 [arXiv:astro- ph/0111408 [astro-ph]]
2002 doi
-
[24]
A precision calculation of relic neutrino decoupling,
K. Akita and M. Yamaguchi, “A precision calculation of relic neutrino decoupling,” JCAP08, 012 (2020) doi:10.1088/1475-7516/2020/08/012 [arXiv:2005.07047 [hep-ph]]
2020 doi
-
[25]
To- wards a precision calculation ofN eff in the Stan- dard Model II: Neutrino decoupling in the presence of flavour oscillations and finite-temperature QED,
J. J. Bennett, G. Buldgen, P. F. De Salas, M. Drewes, S. Gariazzo, S. Pastor and Y. Y. Y. Wong, “To- wards a precision calculation ofN eff in the Stan- dard Model II: Neutrino decoupling in the presence of flavour oscillations and finite-temperature QED,” JCAP 04, 073 (2021) d...
2021 doi
-
[27]
The synergy between CMB spectral distortions and anisotropies,
M. Lucca, N. Sch¨ oneberg, D. C. Hooper, J. Les- gourgues and J. Chluba, “The synergy between CMB spectral distortions and anisotropies,” JCAP 02, 026 (2020) doi:10.1088/1475-7516/2020/02/026 [arXiv:1910.04619 [astro-ph.CO]]
2020 doi
-
[28]
Su- pernova 1987A Constraints on Sub-GeV Dark Sec- tors, Millicharged Particles, the QCD Axion, and an Axion-like Particle,
J. H. Chang, R. Essig and S. D. McDermott, “Su- pernova 1987A Constraints on Sub-GeV Dark Sec- tors, Millicharged Particles, the QCD Axion, and an Axion-like Particle,” JHEP09, 051 (2018) doi:10.1007/JHEP09(2018)051 [arXiv:1803.00993 [hep- ph]]
2018 doi
-
[29]
Abundance and properties of dark radi- ation from the cosmic microwave background,
M. M. Saravanan, T. Brinckmann, M. Loverde and Z. J. Weiner, “Abundance and properties of dark radi- ation from the cosmic microwave background,” JCAP 08(2025), 040 doi:10.1088/1475-7516/2025/08/040 [arXiv:2503.04671 [astro-ph.CO]]
2025 doi
-
[30]
The Cosmic Lin- ear Anisotropy Solving System (CLASS) IV: ef- ficient implementation of non-cold relics,
J. Lesgourgues and T. Tram, “The Cosmic Lin- ear Anisotropy Solving System (CLASS) IV: ef- ficient implementation of non-cold relics,” JCAP 09, 032 (2011) doi:10.1088/1475-7516/2011/09/032 [arXiv:1104.2935 [astro-ph.CO]]
2011 doi
-
[31]
Fast, differentiable, and extensible big bang nucleosynthesis package,
C. Giovanetti, M. Lisanti, H. Liu, S. Mishra-Sharma and J. T. Ruderman, “Fast, differentiable, and extensible big bang nucleosynthesis package,” Phys. Rev. D112, no.6, 063531 (2025) doi:10.1103/f3tj-r882 [arXiv:2408.14538 10 [astro-ph.CO]]
2025 doi
-
[32]
Neutrino decoupling beyond the Stan- dard Model: CMB constraints on the Dark Matter mass with a fast and preciseN eff evaluation,
M. Escudero, “Neutrino decoupling beyond the Stan- dard Model: CMB constraints on the Dark Matter mass with a fast and preciseN eff evaluation,” JCAP 02, 007 (2019) doi:10.1088/1475-7516/2019/02/007 [arXiv:1812.05605 [hep-ph]]
2019 doi
-
[33]
Precision early universe ther- modynamics made simple:N eff and neutrino decou- pling in the Standard Model and beyond,
M. Escudero Abenza, “Precision early universe ther- modynamics made simple:N eff and neutrino decou- pling in the Standard Model and beyond,” JCAP 05, 048 (2020) doi:10.1088/1475-7516/2020/05/048 [arXiv:2001.04466 [hep-ph]]
2020 doi
-
[34]
Precision big bang nucleosynthesis with improved Helium-4 predictions,
C. Pitrou, A. Coc, J. P. Uzan and E. Vangioni, “Precision big bang nucleosynthesis with improved Helium-4 predictions,” Phys. Rept.754, 1-66 (2018) doi:10.1016/j.physrep.2018.04.005 [arXiv:1801.08023 [astro-ph.CO]]
2018 doi
-
[35]
PRyMor- dial: the first three minutes, within and beyond the standard model,
A. K. Burns, T. M. P. Tait and M. Valli, “PRyMor- dial: the first three minutes, within and beyond the standard model,” Eur. Phys. J. C84, no.1, 86 (2024) doi:10.1140/epjc/s10052-024-12442-0 [arXiv:2307.07061 [hep-ph]]
2024 doi
-
[36]
Nested Sampling,
J. Skilling, “Nested Sampling,” AIP Conf. Proc.735, 395 (2004) doi:10.1063/1.1835238
2004 doi
-
[37]
Nested sampling for general Bayesian computation,
J. Skilling, “Nested sampling for general Bayesian computation,” Bayesian Anal.1, no.4, 833 (2006) doi:10.1214/06-BA127
2006 doi
-
[38]
Dynamic nested sampling: an improved algorithm for parameter estimation and evidence calculation,
E. Higson, W. Handley, M. Hobson and A. Lasenby, “Dynamic nested sampling: an improved algorithm for parameter estimation and evidence calculation,” Stat. Comput.29, no.5, 891-913 (2018) doi:10.1007/s11222- 018-9844-0 [arXiv:1704.03459 [stat.CO]]
2018 doi
-
[39]
dynesty: a dynamic nested sampling package for estimating Bayesian posteriors and ev- idences,
J. S. Speagle, “dynesty: a dynamic nested sampling package for estimating Bayesian posteriors and ev- idences,” Mon. Not. Roy. Astron. Soc.493, 3132 (2020) doi:10.1093/mnras/staa278 [arXiv:1904.02180 [astro-ph.IM]]
2020 doi
-
[40]
dynesty: v3.0.0,
S. Koposovet al., “dynesty: v3.0.0,” (2023), doi.org/10.5281/zenodo.3348367
2023 doi
-
[41]
Planck 2018 results. V. CMB power spectra and likelihoods,
N. Aghanimet al.[Planck], “Planck 2018 results. V. CMB power spectra and likelihoods,” Astron. Astro- phys.641, A5 (2020) doi:10.1051/0004-6361/201936386 [arXiv:1907.12875 [astro-ph.CO]]
2018 doi
-
[43]
The LBT Y p Project IV: A New Value of the Primordial Helium Abun- dance,
E. Aver, E. D. Skillman, R. W. Pogge, N. S. J. Rogers, M. K. Weller, K. A. Olive, D. A. Berg, J. J. Salzer, J. H. Miller and J. E. M´ endez-Delgado, “The LBT Y p Project IV: A New Value of the Primordial Helium Abun- dance,” [arXiv:2601.22238 [astro-ph.CO]]
-
[44]
One Percent Determination of the Primordial Deuterium Abundance,
R. J. Cooke, M. Pettini and C. C. Steidel, “One Percent Determination of the Primordial Deuterium Abundance,” Astrophys. J.855, no.2, 102 (2018) doi:10.3847/1538-4357/aaab53 [arXiv:1710.11129 [astro- ph.CO]]
2018 doi
-
[45]
A new tension in the cosmological model from pri- mordial deuterium?,
C. Pitrou, A. Coc, J. P. Uzan and E. Vangioni, “A new tension in the cosmological model from pri- mordial deuterium?,” Mon. Not. Roy. Astron. Soc. 502, no.2, 2474-2481 (2021) doi:10.1093/mnras/stab135 [arXiv:2011.11320 [astro-ph.CO]]
2021 doi
-
[47]
Pri- mordial Deuterium after LUNA: concordances and er- ror budget,
O. Pisanti, G. Mangano, G. Miele and P. Mazzella, “Pri- mordial Deuterium after LUNA: concordances and er- ror budget,” JCAP04, 020 (2021) doi:10.1088/1475- 7516/2021/04/020 [arXiv:2011.11537 [astro-ph.CO]]
2021 doi
-
[48]
Cos- mological constraints on light but massive relics,
W. L. Xu, J. B. Mu˜ noz and C. Dvorkin, “Cos- mological constraints on light but massive relics,” Phys. Rev. D105, no.9, 095029 (2022) doi:10.1103/PhysRevD.105.095029 [arXiv:2107.09664 [astro-ph.CO]]
2022 doi
-
[49]
Clustering with Light (but Massive) Relics,
J. Kumar, P. Sandick and S. Xu, “Clustering with Light (but Massive) Relics,” [arXiv:2512.14672 [astro-ph.CO]]. Appendix A: Derivation of Comoving Energy Density Ratios We derive here analytic approximations for the quantitiesr,r γ, andr ur defined in Section II. We work in th...
1921
Reviewed May 10, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.