Evaporation of primordial black holes with multimodal mass and extended spin distributions: cosmological imprints on the effective number of relativistic species

Abstract Primordial black holes (PBHs) form through several distinct mechanisms, each imprinting a characteristic mass function that a single-mass treatment risks erasing. Building on the code, we introduce ( https://doi.org/10.5281/zenodo.22699162 ), implementing four mass functions – log-normal, power-law, critical collapse, metric preheating – in a multimodal framework, with spin modeled via Gaussian and Fishbach et al. profiles. Crucially, each channel’s weight is derived from the primordial collapse probability rather than fitted, tying the mass function to the power-spectrum amplitude – a concrete link between inflationary model-building and CMB observables. Solving the Friedmann–Boltzmann equations for $$M_\textrm{PBH}^\textrm{in}=10^{7}$$ M PBH in = 10 7 g in the pre-BBN window, we compute $$\varDelta N_\textrm{eff}$$ Δ N eff for five distributions, three spin configurations, and three weighting scenarios. Extended mass functions enhance $$\varDelta N_\textrm{eff}$$ Δ N eff over the monochromatic benchmark by factors of $$\sim \!1.03$$ ∼ 1.03 (critical collapse) to $$\sim \!1.84$$ ∼ 1.84 (log-normal), preserving the hierarchy $$LN> MM> PL> MP > CC$$ L N > M M > P L > M P > C C across the mass window $$\{10^{5},10^{7},10^{8}\}$$ { 10 5 , 10 7 , 10 8 } g. Near-extremal spin ( $$a_{\star }=0.99$$ a ⋆ = 0.99 ) and spin-2 dark radiation invert this trend: superradiant spin loss averages away faster in broad distributions than in a monochromatic population, letting the monochromatic approximation overestimate $$\varDelta N_\textrm{eff}$$ Δ N eff . Against CMB-S4 and Simons Observatory sensitivities ( $$\sigma \simeq 0.06$$ σ ≃ 0.06 and 0.05), the monochromatic benchmark is undetectable for scalar dark radiation (sDR $$=0$$ = 0

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Journal
The European Physical Journal C
Published
2026-09-20
DOI
https://doi.org/10.1140/epjc/s10052-026-16372-x
Primary Topic
Cosmology and Gravitation Theories
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article
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article

Evaporation of primordial black holes with multimodal mass and extended spin distributions: cosmological imprints on the effective number of relativistic species

A. Daassou, Y. Ouchhaine, T. Toghrai, R. Benbrik et al.
The European Physical Journal C
Cosmology and Gravitation Theories
article

Evaporation of primordial black holes with multimodal mass and extended spin distributions: cosmological imprints on the effective number of relativistic species

A. Daassou, Y. Ouchhaine, T. Toghrai, R. Benbrik, H. Laassiri
article en

Abstract

Abstract Primordial black holes (PBHs) form through several distinct mechanisms, each imprinting a characteristic mass function that a single-mass treatment risks erasing. Building on the code, we introduce ( https://doi.org/10.5281/zenodo.22699162 ), implementing four mass functions – log-normal, power-law, critical collapse, metric preheating – in a multimodal framework, with spin modeled via Gaussian and Fishbach et al. profiles. Crucially, each channel’s weight is derived from the primordial collapse probability rather than fitted, tying the mass function to the power-spectrum amplitude – a concrete link between inflationary model-building and CMB observables. Solving the Friedmann–Boltzmann equations for $$M_\textrm{PBH}^\textrm{in}=10^{7}$$ M PBH in = 10 7 g in the pre-BBN window, we compute $$\varDelta N_\textrm{eff}$$ Δ N eff for five distributions, three spin configurations, and three weighting scenarios. Extended mass functions enhance $$\varDelta N_\textrm{eff}$$ Δ N eff over the monochromatic benchmark by factors of $$\sim \!1.03$$ ∼ 1.03 (critical collapse) to $$\sim \!1.84$$ ∼ 1.84 (log-normal), preserving the hierarchy $$LN> MM> PL> MP > CC$$ L N > M M > P L > M P > C C across the mass window $$\{10^{5},10^{7},10^{8}\}$$ { 10 5 , 10 7 , 10 8 } g. Near-extremal spin ( $$a_{\star }=0.99$$ a ⋆ = 0.99 ) and spin-2 dark radiation invert this trend: superradiant spin loss averages away faster in broad distributions than in a monochromatic population, letting the monochromatic approximation overestimate $$\varDelta N_\textrm{eff}$$ Δ N eff . Against CMB-S4 and Simons Observatory sensitivities ( $$\sigma \simeq 0.06$$ σ ≃ 0.06 and 0.05), the monochromatic benchmark is undetectable for scalar dark radiation (sDR $$=0$$ = 0

The European Physical Journal CVol. 86(9)
Cadi Ayyad University (MA)
Openalex Percentile: Top 23%
Cosmology and Gravitation Theories
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