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Cosmology and Nongalactic AstrophysicsEnglishPublished

Rayleigh scattering of cosmic‑background photons by neutral hydrogen and helium leaves a frequency‑dependent imprint on the microwave sky

November 14, 2026arXiv: 2611.17209v1

A team of cosmologists has shown that as the universe recombined, neutral hydrogen and helium scattered cosmic‑microwave background (CMB) photons through Rayleigh scattering (RS). The effect adds a part of the CMB anisotropies that grows like the fourth power of frequency (ν⁴) at leading order and peaks between 200 GHz and 800 GHz.

To assess how useful this signal could be, the researchers performed a multi‑frequency Fisher‑matrix forecast that included realistic noise and foreground models. They simulated two next‑generation CMB experiments – the proposed PICO satellite and a combination of LiteBIRD with the existing Planck data – and measured how the additional RS contribution would tighten constraints on cosmological parameters. For the standard ΛCDM cosmology, adding RS improves the constraints on all parameters by at most 7 % for PICO and by less than 2 % for LiteBIRD + Planck.

However, when the analysis allows the electron mass (m_e) or the fine‑structure constant (α) to vary during recombination – scenarios motivated by attempts to resolve the present Hubble‑tension – the improvement can reach roughly 31 % for key parameters such as the Hubble constant, m_e, α, the baryon density Ω_b h², and the cold‑dark‑matter density Ω_c h².

The study also quantified the danger of ignoring RS. Neglecting the signal biases the inferred cosmological parameters by up to about one standard deviation for PICO and by less than one σ for LiteBIRD + Planck. This level of bias shows that future analyses of CMB data must include RS to avoid systematic errors.

Figure 2 in the paper depicts how changing m_e or α shifts the Rayleigh opacity as a function of redshift and frequency, confirming the ν⁴ scaling predicted for the RS signal. Table 1 lists the foreground components that were modeled in the forecast, illustrating the complexity of the covariance matrix and the importance of accurate foreground simulations for robust parameter estimation.

Diagram showing how small changes in the electron mass and fine‑structure constant alter the Rayleigh scattering opacity as a function of redshift at two observing frequencies, highlighting the frequency dependence and the impact on cosmological parameter constraints. (1/2)Diagram showing how small changes in the electron mass and fine‑structure constant alter the Rayleigh scattering opacity as a function of redshift at two observing frequencies, highlighting the frequency dependence and the impact on cosmological parameter constraints. (2/2)
Figure 2. Effects of changing electron mass (Δ me/me = −0.1 and +0.1) and fine‑structure constant (Δ α/α = −0.1 and +0.1) on the Rayleigh comoving opacity, τ̇R(ν), plotted versus redshift. The left panel shows the dependence on Δ me/me at 321 GHz (dash-dotted) and 799 GHz (dashed) with the ΛCDM curve highlighted in grey. The right panel reproduces the same for Δ α/α. The figure demonstrates the ν⁴ scaling of Rayleigh scattering and the improvement of parameter constraints when these constants vary.Adak, Debabrata, Vanetti, Elena, Génova-Santos, R. T., Chluba, Jens, Hernández-Monteagudo, Carlos, Rubiño-Mart\'ın, J. A. · arXiv:2611.17209v1 · Figure 2: · CC BY 4.0
Table listing the foreground sources modeled in the survey, each with its spectral model, fiducial amplitude, and reference.
ComponentSpectraModel, Dℓνi​νj [μ​K2]Fiducial parametersReferences
kSZT​TakSZ​Dℓ,ℓ0kSZakSZ=1.48Battaglia et al. (2013); Louis et al. (2025)
tSZT​TatSZ​Dℓ,ℓ0tSZ​(ℓℓ0)αtSZ​f⁡(νi)​f​(νj)f2​(ν0)atSZ=3.3, αtSZ=−0.53Battaglia et al. (2012); Louis et al. (2025)
CIB, PoissonT​Tap​ℓ⁡(ℓ+1)ℓ0​(ℓ0+1)​μ⁡(νi,βp,Td)​μ​(νj,βp,Td)μ2​(ν0,βp,Td)ap=7.65, βp=1.87, Td=9.6KLouis et al. (2025); Beringue et al. (2025)
CIB, clusteredT​Tac​Dℓ,ℓ0CIB​-​c​μ⁡(νi,βc,Td)​μ​(νj,βc,Td)μ2​(ν0,βc,Td)ac=3.69, βc=1.87Planck Collaboration et al. (2014); Choi et al. (2020)
tSZ×CIBT​T−ξ​atSZ​ac​Dℓ,ℓ0tSZ×CIB​f⁡(νi)​μ​(νj,βc,Td)+f⁡(νj)​μ​(νi,βc,Td)f⁡(ν0)​μ​(ν0,βc,Td)ξ=0.09Addison et al. (2012); Louis et al. (2025)
Radio sourcesT​Tas​ℓ⁡(ℓ+1)ℓ0​(ℓ0+1)​(νi​νjν02)βs​g⁡(νi)​g​(νj)g2​(ν0)as=2.86, βs=−2.5Dunkley et al. (2011); Louis et al. (2025); Beringue et al. (2025)
Galactic dustT​T, T​E, E​EagX​Y​(ℓ500)αdX​Y​μ⁡(νi,βd,Tdeff)​μ​(νj,βd,Tdeff)μ2​(ν0,βd,Tdeff)agT​T=7.9, agT​E=0.42, agE​E=0.167, αdT​T=−0.6, αdT​E,E​E=−0.4, βd=1.5, Tdeff=19.6KPlanck Collaboration et al. (2020c); Louis et al. (2025)
SynchrotronT​T, E​EasyncX​X​(ℓ80)αsync​(νi​νjν02)βsync​g⁡(νi)​g​(νj)g2​(ν0), ν0=30GHzasyncT​T=9.8, asyncE​E=2.37, αsync=−0.81, βsync=−3.1Planck Collaboration et al. (2020d)
Table 1. Foreground components and their fiducial parameters used in the Fisher‑matrix forecast for PICO and LiteBIRD + Planck.Adak, Debabrata, Vanetti, Elena, Génova-Santos, R. T., Chluba, Jens, Hernández-Monteagudo, Carlos, Rubiño-Mart\'ın, J. A. · arXiv:2611.17209v1 · Table 1: · CC BY 4.0

Source paper

Shedding light on modified recombination scenarios with Rayleigh scattering of the CMB

Cosmology and Nongalactic Astrophysics
View on arXiv
Rayleigh scattering of cosmic‑background photons by neutral hydrogen and helium leaves a frequency‑dependent imprint on the microwave sky | arXiv News