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Research PaperResearchia:202610.09015

Partially Thermalized eV-Scale Sterile Neutrinos in Dynamical Dark Energy and Non-Flat Cosmologies

Gopal Kashyap

Abstract

We investigate cosmological constraints on a $(3+1)$ neutrino framework containing an additional partially thermalized, eV-scale sterile neutrino alongside the three active species. Rather than assuming full thermalization, we allow the sterile abundance to vary independently through its physical mass $m_s$ and contribution $ΔN_{\rm eff}$ to the effective number of relativistic species. The sterile state is modeled as a thermally distributed non-cold relic with a temperature below that of the ac...

Submitted: October 9, 2026Subjects: Physics; Physics

Description / Details

We investigate cosmological constraints on a (3+1)(3+1) neutrino framework containing an additional partially thermalized, eV-scale sterile neutrino alongside the three active species. Rather than assuming full thermalization, we allow the sterile abundance to vary independently through its physical mass msm_s and contribution ΔNeffΔN_{\rm eff} to the effective number of relativistic species. The sterile state is modeled as a thermally distributed non-cold relic with a temperature below that of the active-neutrino background. We consider flat and non-flat ΛΛCDM and w0waw_0w_aCDM cosmologies, all including the same (3+1)ν(3+1)ν sector. The models are constrained using Planck 2018 CMB data, DESI DR2 BAO, Pantheon+ Type Ia supernovae, a conservative compilation of fσ8fσ_8 measurements, and the recent H0DN. Oscillation-informed priors are imposed on the active-neutrino mass splittings, while the eV scale sterile-mass range is motivated by short-baseline oscillation searches and global (3+1)(3+1) analyses. We find that allowing additional freedom in the late-time cosmological background substantially changes the inferred sterile-neutrino sector. The effective sterile mass increases from ms,eff∼0.11±0.05 eVm_{s,\rm eff}\sim0.11\pm0.05~{\rm eV} in flat ΛΛCDM+(3+1)ν+(3+1)ν to ∼0.35±0.12 eV\sim0.35\pm0.12~{\rm eV} in the non-flat w0waw_0w_aCDM+(3+1)ν+(3+1)ν model. The corresponding sterile abundance shifts from ΔNeff≲0.1ΔN_{\rm eff}\lesssim0.1 to ΔNeff≃0.35±0.15ΔN_{\rm eff}\simeq0.35\pm0.15, while remaining well below the fully thermalized limit, ΔNeff≃1ΔN_{\rm eff}\simeq1. The non-flat w0waw_0w_aCDM models also show ∼2.8σ\sim 2.8σ preference for open spatial geometry, Ωk≃0.0045±0.0016Ω_k\simeq0.0045\pm0.0016, and yield H0≃70.9±0.7 km s−1 Mpc−1H_0\simeq70.9\pm0.7~{\rm km\,s^{-1}\,Mpc^{-1}} and S8≃0.785±0.015S_8\simeq0.785\pm0.015. These models improve the minimum χ2χ^2 by approximately 2121-2525 relative to flat ΛΛCDM+(3+1)ν+(3+1)ν.


Source: arXiv:2610.10585v1 - http://arxiv.org/abs/2610.10585v1 PDF: https://arxiv.org/pdf/2610.10585v1 Original Link: http://arxiv.org/abs/2610.10585v1

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Date:
Oct 9, 2026
Topic:
Physics
Area:
Physics
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