Consistent N_{rm eff} fitting in big bang nucleosynthesis analysis
Pith reviewed 2026-05-19 02:44 UTC · model grok-4.3
The pith
BBN constraints on negative N_eff deviate when entropy injection is modeled after neutrino decoupling.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Under the assumption that negative Delta N_eff arises from entropy injection into the electromagnetic sector after neutrino decoupling, the resulting BBN constraints on N_eff deviate significantly from those obtained by the conventional extrapolation of dark radiation scenarios into the Delta N_eff < 0 regime. This process dilutes the neutrino density and suppresses the rate of neutrino-driven neutron-proton conversion.
What carries the argument
Entropy injection into the electromagnetic sector after neutrino decoupling, which dilutes the neutrino temperature relative to photons and suppresses neutrino-induced n-p conversion rates.
If this is right
- The allowed range of N_eff must be restricted or neutrino reaction rates adjusted according to the physical scenario for consistent BBN analysis.
- BBN constraints become scenario-dependent rather than universally applicable for negative Delta N_eff.
- This affects the interpretation of cosmological observations in the presence of new physics that injects entropy post-decoupling.
Where Pith is reading between the lines
- Future studies of decaying particles should use this adjusted approach to derive more accurate BBN limits.
- The method could be extended to other post-decoupling processes affecting neutrino-photon temperature ratios.
- It connects to the broader problem of consistently parametrizing deviations in effective degrees of freedom across different epochs.
Load-bearing premise
The entropy injection is assumed to occur after neutrino decoupling, affecting only the electromagnetic sector and thereby diluting neutrinos relative to photons while suppressing their interaction rates.
What would settle it
Precise measurements of primordial helium-4 and deuterium abundances that distinguish between the adjusted neutrino rates and the conventional negative Delta N_eff extrapolation.
Figures
read the original abstract
The effective number of neutrino species, $N_{\rm eff}$, serves as a key fitting parameter extensively employed in cosmological studies. In this work, we point out a fundamental inconsistency in the conventional treatment of $N_{\rm eff}$ in big bang nucleosynthesis (BBN), particularly regarding its applicability to new physics scenarios where $\Delta N_{\rm eff}$, the deviation of $N_{\rm eff}$ from the standard BBN prediction, is negative. To ensure consistent interpretation, it is imperative to either restrict the allowed range of $N_{\rm eff}$ or systematically adjust neutrino-induced reaction rates based on physically motivated assumptions. As a concrete example, we consider a simple scenario in which a negative $\Delta N_{\rm eff}$ arises from entropy injection into the electromagnetic sector due to the decay of long-lived particles after neutrino decoupling. This process dilutes the neutrino density and suppresses the rate of neutrino-driven neutron-proton conversion. Under this assumption, we demonstrate that the resulting BBN constraints on $N_{\rm eff}$ deviate significantly from those obtained by the conventional, but unphysical, extrapolation of dark radiation scenarios into the $\Delta N_{\rm eff} < 0$ regime.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that conventional N_eff fitting in BBN is inconsistent for negative Delta N_eff because it simply reduces total radiation density without accounting for changes to neutrino temperature or weak rates. Using the concrete example of entropy injection into the electromagnetic sector from long-lived particle decays after neutrino decoupling, the authors argue that this physically motivated scenario dilutes the neutrino-to-photon temperature ratio and suppresses neutrino-induced n-p conversion rates, leading to BBN constraints on N_eff that deviate significantly from those obtained by extrapolating dark-radiation models into the Delta N_eff < 0 regime.
Significance. If the quantitative demonstration is robust, the result would be significant for BBN analyses of new-physics scenarios that produce negative Delta N_eff, as it shows that unphysical extrapolations can bias constraints on primordial abundances and thereby affect interpretations of cosmological data.
major comments (2)
- [Abstract] The central claim that constraints 'deviate significantly' rests on the post-decoupling entropy-injection scenario, yet the manuscript presents this only as an illustrative example without deriving the required rescaling of the weak rates from the Boltzmann equations or from an explicit particle Lagrangian (see abstract and the discussion of the concrete scenario).
- To establish that the modified Hubble rate and adjusted weak rates produce quantitatively different abundance predictions, the paper must show the effect on the n-p conversion rates and the resulting shifts in Y_p or D/H; without these explicit calculations or comparison plots, the size of the reported deviation cannot be verified as robust against changes in decay lifetime, branching ratio, or injection epoch.
minor comments (1)
- Clarify in the introduction whether the standard N_eff = 3.046 value is held fixed or allowed to vary when comparing the two fitting procedures.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments on our manuscript. We appreciate the opportunity to clarify the scope of our illustrative example and to strengthen the quantitative presentation of the results. We address each major comment below and indicate the revisions we will implement.
read point-by-point responses
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Referee: [Abstract] The central claim that constraints 'deviate significantly' rests on the post-decoupling entropy-injection scenario, yet the manuscript presents this only as an illustrative example without deriving the required rescaling of the weak rates from the Boltzmann equations or from an explicit particle Lagrangian (see abstract and the discussion of the concrete scenario).
Authors: The entropy-injection scenario serves as a concrete illustrative example to demonstrate the physical inconsistency of extrapolating conventional N_eff fits into the negative Delta N_eff regime. The rescaling of the weak rates follows from the standard entropy dilution that reduces the neutrino-to-photon temperature ratio after decoupling, which directly suppresses the phase-space density entering the n-p conversion rates. This is a general consequence of post-decoupling EM entropy production and does not depend on a specific particle Lagrangian. To address the concern, we will add a concise derivation of the temperature ratio and the resulting Boltzmann-equation adjustment to the weak rates in the revised manuscript. revision: yes
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Referee: [—] To establish that the modified Hubble rate and adjusted weak rates produce quantitatively different abundance predictions, the paper must show the effect on the n-p conversion rates and the resulting shifts in Y_p or D/H; without these explicit calculations or comparison plots, the size of the reported deviation cannot be verified as robust against changes in decay lifetime, branching ratio, or injection epoch.
Authors: The BBN abundance calculations in the manuscript already incorporate both the modified Hubble rate and the adjusted weak rates for the entropy-injection example, yielding the reported deviation from conventional fits. To make the quantitative impact explicit and allow verification of robustness, we will include new figures in the revised version showing the n-p conversion rates as a function of temperature for the standard and modified cases, together with the resulting shifts in Y_p and D/H for representative values of decay lifetime, branching ratio, and injection epoch. revision: yes
Circularity Check
No significant circularity in the N_eff BBN consistency analysis
full rationale
The paper contrasts the conventional extrapolation of N_eff into the negative Delta N_eff regime (which simply reduces total radiation density) against an explicit illustrative scenario of post-neutrino-decoupling entropy injection into the EM sector from long-lived particle decay. This scenario is used to adjust both the Hubble expansion rate and the neutrino-induced n-p conversion rates, with the resulting abundance predictions computed numerically and shown to differ. No load-bearing step reduces by construction to a fitted input, self-citation chain, or ansatz smuggled from prior work; the modeling choice is stated as a concrete example rather than derived as a uniqueness theorem, and the central claim remains an independent numerical comparison against standard BBN codes. The derivation is therefore self-contained.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Neutrino decoupling occurs before the entropy injection from long-lived particle decay
Lean theorems connected to this paper
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
negative ΔN_eff arises from entropy injection into the electromagnetic sector after neutrino decoupling... dilutes the neutrino density and suppresses the rate of neutrino-driven neutron-proton conversion
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Tν(Tγ)/T(0)ν(Tγ) = (Neff/N(0)eff)1/4 for ΔN_eff < 0
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]
We recommend not to use Neff in BBN analysis
Neff is not a good fitting parameter in the BBN analysis. We recommend not to use Neff in BBN analysis
-
[2]
If it is insisted to use Neff, some model dependence is inevitable. One may simply include minimal cor- rections in the neutrino-induced n ↔ p conversion rates for ∆ Neff < 0, but it does not give a mean- ingful result in the end, as shown in Fig. 1. Fig. 1 shows our fitting result in the Ω bh2 – Neff plane obtained with the simplest assumption on neutrin...
-
[3]
∆Neff < 0 For negative ∆Neff, the deviation is realized via a re- duction in the neutrino temperature, as described by Eq. (6). To linear order, this gives δTν T (0) ν ≃ 1 12∆Neff . (18) This in turn modifies the Hubble rate as H ≃ H(0) 1 + 42 43 δTν T (0) ν . (19) Since the neutron-proton conversion rates are sensitive to the electron-neutrino temperatur...
-
[4]
∆Neff > 0 In the case of positive ∆ Neff, corresponding to ad- ditional dark radiation degree, the neutron-proton con- version rates are unchanged from the SBBN case (i.e., Tν = T (0) ν ). The change in H then leads to a shift in the freeze-out temperature as δTnp T (0) np ≃ 3 × 10−2∆Neff (29) This results in a modified freeze-out abundance δXn,fo X(0) n,...
- [5]
- [6]
-
[7]
G. Mangano, G. Miele, S. Pastor, and M. Peloso, A Pre- cision calculation of the effective number of cosmologi- cal neutrinos, Phys. Lett. B 534, 8 (2002), arXiv:astro- ph/0111408
-
[8]
Relic neutrino decoupling including flavour oscillations
G. Mangano, G. Miele, S. Pastor, T. Pinto, O. Pisanti, and P. D. Serpico, Relic neutrino decoupling includ- ing flavor oscillations, Nucl. Phys. B 729, 221 (2005), arXiv:hep-ph/0506164
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[9]
P. F. de Salas and S. Pastor, Relic neutrino decou- pling with flavour oscillations revisited, JCAP 07, 051, arXiv:1606.06986 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
-
[10]
M. Escudero Abenza, Precision early universe thermo- dynamics made simple: Neff and neutrino decoupling in the Standard Model and beyond, JCAP 05, 048, arXiv:2001.04466 [hep-ph]
-
[11]
K. Akita and M. Yamaguchi, A precision calcula- tion of relic neutrino decoupling, JCAP 08, 012, arXiv:2005.07047 [hep-ph]
- [12]
-
[13]
A Lower Bound on the Mass of Cold Thermal Dark Matter from Planck
C. Boehm, M. J. Dolan, and C. McCabe, A Lower Bound on the Mass of Cold Thermal Dark Matter from Planck, JCAP 08, 041, arXiv:1303.6270 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
-
[14]
Dark Radiation constraints on minicharged particles in models with a hidden photon
H. Vogel and J. Redondo, Dark Radiation constraints on minicharged particles in models with a hidden photon, JCAP 02, 029, arXiv:1311.2600 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv
-
[15]
M. A. Buen-Abad, G. Marques-Tavares, and M. Schmaltz, Non-Abelian dark matter and dark radia- tion, Phys. Rev. D 92, 023531 (2015), arXiv:1505.03542 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[16]
A Hidden Dark Matter Sector, Dark Radiation, and the CMB
Z. Chacko, Y. Cui, S. Hong, and T. Okui, Hidden dark matter sector, dark radiation, and the CMB, Phys. Rev. D 92, 055033 (2015), arXiv:1505.04192 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2015
- [17]
-
[18]
C. Giovanetti, M. Lisanti, H. Liu, and J. T. Ruderman, Joint Cosmic Microwave Background and Big Bang Nu- cleosynthesis Constraints on Light Dark Sectors with Dark Radiation, Phys. Rev. Lett. 129, 021302 (2022), arXiv:2109.03246 [hep-ph]
-
[19]
P. Adshead, P. Ralegankar, and J. Shelton, Dark radia- tion constraints on portal interactions with hidden sec- tors, JCAP 09, 056, arXiv:2206.13530 [hep-ph]
-
[20]
R. L. Workman et al. (Particle Data Group), Review of Particle Physics, PTEP 2022, 083C01 (2022)
work page 2022
-
[21]
The Atacama Cosmology Telescope: DR6 Constraints on Extended Cosmological Models
E. Calabrese et al. (ACT), The Atacama Cosmology Tele- scope: DR6 Constraints on Extended Cosmological Mod- els, (2025), arXiv:2503.14454 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[22]
Planck 2018 results. VI. Cosmological parameters
N. Aghanim et 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]
work page internal anchor Pith review Pith/arXiv arXiv 2018
- [23]
- [24]
- [25]
-
[26]
M. H. Reno and D. Seckel, Primordial Nucleosynthesis: The Effects of Injecting Hadrons, Phys. Rev. D 37, 3441 (1988)
work page 1988
-
[27]
K. Kohri and J. Yokoyama, Primordial black holes and primordial nucleosynthesis. 1. Effects of hadron injection from low mass holes, Phys. Rev. D 61, 023501 (2000), arXiv:astro-ph/9908160
work page internal anchor Pith review Pith/arXiv arXiv 2000
-
[28]
Primordial nucleosynthesis and hadronic decay of a massive particle with a relatively short lifetime
K. Kohri, Primordial nucleosynthesis and hadronic decay of a massive particle with a relatively short lifetime, Phys. Rev. D 64, 043515 (2001), arXiv:astro-ph/0103411
work page internal anchor Pith review Pith/arXiv arXiv 2001
-
[29]
Metastable GeV-scale particles as a solution to the cosmological lithium problem
M. Pospelov and J. Pradler, Metastable GeV-scale par- ticles as a solution to the cosmological lithium problem, Phys. Rev. D 82, 103514 (2010), arXiv:1006.4172 [hep- ph]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[30]
Cosmology With a Very Light $L_\mu - L_\tau$ Gauge Boson
M. Escudero, D. Hooper, G. Krnjaic, and M. Pierre, Cos- mology with A Very Light Lµ − Lτ Gauge Boson, JHEP 03, 071, arXiv:1901.02010 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 1901
- [31]
-
[32]
H. Esseili and G. D. Kribs, Cosmological implications of gauged U(1)B−L on ∆N ef f in the CMB and BBN, JCAP 05, 110, arXiv:2308.07955 [hep-ph]
- [33]
- [34]
-
[35]
Cosmological Constraints on Neutrino Injection
T. Kanzaki, M. Kawasaki, K. Kohri, and T. Moroi, Cos- mological Constraints on Neutrino Injection, Phys. Rev. D 76, 105017 (2007), arXiv:0705.1200 [hep-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2007
- [36]
-
[37]
E. W. Kolb and M. S. Turner, The Early Universe , Vol. 69 (1990)
work page 1990
- [38]
- [39]
-
[40]
S. Navas et al. (Particle Data Group), Review of particle physics, Phys. Rev. D 110, 030001 (2024)
work page 2024
-
[41]
PArthENoPE: Public Algorithm Evaluating the Nucleosynthesis of Primordial Elements
O. Pisanti, A. Cirillo, S. Esposito, F. Iocco, G. Mangano, G. Miele, and P. D. Serpico, PArthENoPE: Public Al- gorithm Evaluating the Nucleosynthesis of Primordial Elements, Comput. Phys. Commun. 178, 956 (2008), 8 arXiv:0705.0290 [astro-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[42]
R. Consiglio, P. F. de Salas, G. Mangano, G. Miele, S. Pastor, and O. Pisanti, PArthENoPE reloaded, Com- put. Phys. Commun. 233, 237 (2018), arXiv:1712.04378 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[43]
S. Gariazzo, P. F. de Salas, O. Pisanti, and R. Consiglio, PArthENoPE revolutions, Comput. Phys. Commun. 271, 108205 (2022), arXiv:2103.05027 [astro-ph.IM]
-
[44]
P. D. Serpico, S. Esposito, F. Iocco, G. Mangano, G. Miele, and O. Pisanti, Nuclear reaction network for primordial nucleosynthesis: A Detailed analysis of rates, uncertainties and light nuclei yields, JCAP 12, 010, arXiv:astro-ph/0408076
work page internal anchor Pith review Pith/arXiv arXiv
-
[45]
A. Matsumoto et al. , EMPRESS. VIII. A New Deter- mination of Primordial He Abundance with Extremely Metal-poor Galaxies: A Suggestion of the Lepton Asym- metry and Implications for the Hubble Tension, As- trophys. J. 941, 167 (2022), arXiv:2203.09617 [astro- ph.CO]
- [46]
-
[47]
M. Escudero, A. Ibarra, and V. Maura, Primordial lep- ton asymmetries in the precision cosmology era: Current status and future sensitivities from BBN and the CMB, Phys. Rev. D 107, 035024 (2023), arXiv:2208.03201 [hep- ph]
-
[48]
M. Kawasaki and K. Murai, Lepton asymmetric universe, JCAP 08 (08), 041, arXiv:2203.09713 [hep-ph]
-
[49]
D. Borah and A. Dasgupta, Large neutrino asymmetry from TeV scale leptogenesis, Phys. Rev. D 108, 035015 (2023), arXiv:2206.14722 [hep-ph]
- [50]
discussion (0)
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