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Searching for sterile neutrinos in dynamical dark energy cosmologies

Lu Feng, Jing-Fei Zhang, Xin Zhang

TL;DR

The paper investigates how dynamical dark energy models affect cosmological limits on sterile neutrinos, comparing ΛCDM+$\\nu_s$, $w$CDM+$\\nu_s$, and HDE+$\\nu_s$ using Planck 2015 data plus low-redshift probes with fixed active-neutrino sum $\\sum m_\\nu=0.06$ eV and varying $N_{\\rm eff}$ and $m_{\\nu,{\\rm sterile}}^{\\rm eff}$. It employs CosmoMC for MCMC sampling and uses AIC for model comparison, finding that without growth data only upper limits can be derived, e.g., for Planck+BAO+SN+$H_0$+lensing the bounds are $m_{\\nu,{\\rm sterile}}^{\\rm eff}<0.2675$ eV (ΛCDM), $<0.5313$ eV (wCDM), and $<0.1989$ eV (HDE), with corresponding $N_{\\rm eff}$ limits. The results show $N_{\\rm eff}$ correlates positively with $H_0$, and the dark-energy model materially shifts the sterile-neutrino limits: the $w$CDM case loosens the mass bound while the HDE case tightens it, though HDE is not favored by the overall fit (large ΔAIC) despite easing the $H_0$ tension. The study highlights that dark-energy properties can significantly influence sterile-neutrino constraints and the interpretation of potential extra relativistic species in cosmology.

Abstract

We investigate how the dark energy properties change the cosmological limits on sterile neutrino parameters by using recent cosmological observations. We consider the simplest dynamical dark energy models, the $w$CDM model and the holographic dark energy (HDE) model, to make an analysis. The cosmological observations used in this work include the Planck 2015 CMB temperature and polarization data, the baryon acoustic oscillation data, the type Ia supernova data, the Hubble constant direct measurement data, and the Planck CMB lensing data. We find that, $m_{ν,{\rm{sterile}}}^{\rm{eff}}<0.2675$ eV and $N_{\rm eff}<3.5718$ for $Λ$CDM cosmology, $m_{ν,{\rm{sterile}}}^{\rm{eff}}<0.5313$ eV and $N_{\rm eff}<3.5008$ for $w$CDM cosmology, and $m_{ν,{\rm{sterile}}}^{\rm{eff}}<0.1989$ eV and $N_{\rm eff}<3.6701$ for HDE cosmology, from the constraints of the combination of these data. Thus, without the addition of measurements of growth of structure, only upper limits on both $m_{ν,{\rm{sterile}}}^{\rm{eff}}$ and $N_{\rm eff}$ can be derived, indicating that no evidence of the existence of a sterile neutrino species with eV-scale mass is found in this analysis. Moreover, compared to the $Λ$CDM model, in the $w$CDM model the limit on $m_{ν,{\rm{sterile}}}^{\rm{eff}}$ becomes much looser, but in the HDE model the limit becomes much tighter. Therefore, the dark energy properties could significantly influence the constraint limits of sterile neutrino parameters.

Searching for sterile neutrinos in dynamical dark energy cosmologies

TL;DR

The paper investigates how dynamical dark energy models affect cosmological limits on sterile neutrinos, comparing ΛCDM+, CDM+, and HDE+ using Planck 2015 data plus low-redshift probes with fixed active-neutrino sum eV and varying and . It employs CosmoMC for MCMC sampling and uses AIC for model comparison, finding that without growth data only upper limits can be derived, e.g., for Planck+BAO+SN++lensing the bounds are eV (ΛCDM), eV (wCDM), and eV (HDE), with corresponding limits. The results show correlates positively with , and the dark-energy model materially shifts the sterile-neutrino limits: the CDM case loosens the mass bound while the HDE case tightens it, though HDE is not favored by the overall fit (large ΔAIC) despite easing the tension. The study highlights that dark-energy properties can significantly influence sterile-neutrino constraints and the interpretation of potential extra relativistic species in cosmology.

Abstract

We investigate how the dark energy properties change the cosmological limits on sterile neutrino parameters by using recent cosmological observations. We consider the simplest dynamical dark energy models, the CDM model and the holographic dark energy (HDE) model, to make an analysis. The cosmological observations used in this work include the Planck 2015 CMB temperature and polarization data, the baryon acoustic oscillation data, the type Ia supernova data, the Hubble constant direct measurement data, and the Planck CMB lensing data. We find that, eV and for CDM cosmology, eV and for CDM cosmology, and eV and for HDE cosmology, from the constraints of the combination of these data. Thus, without the addition of measurements of growth of structure, only upper limits on both and can be derived, indicating that no evidence of the existence of a sterile neutrino species with eV-scale mass is found in this analysis. Moreover, compared to the CDM model, in the CDM model the limit on becomes much looser, but in the HDE model the limit becomes much tighter. Therefore, the dark energy properties could significantly influence the constraint limits of sterile neutrino parameters.

Paper Structure

This paper contains 6 sections, 1 equation, 5 figures, 1 table.

Figures (5)

  • Figure 1: The one-dimensional posterior distributions and two-dimensional marginalized contours (68.3% and 95.4% CL) for the $\Lambda$CDM+$\nu_s$ ( red), $w$CDM+$\nu_s$ ( blue), and HDE+$\nu_s$ ( green) models, from the constraints of the Planck TT,TE,EE+lowP+BAO data combination.
  • Figure 2: The one-dimensional posterior distributions and two-dimensional marginalized contours (68.3% and 95.4% CL) for the $\Lambda$CDM+$\nu_s$ ( red), $w$CDM+$\nu_s$ ( blue), and HDE+$\nu_s$ ( green) models, from the constraints of the Planck TT,TE,EE+lowP+BAO+SN+$H_{0}$+lensing data combination.
  • Figure 3: Constraint results for the $w$CDM+$\nu_s$ model from the Planck TT,TE,EE+lowP+BAO data combination and the Planck TT,TE,EE+lowP+BAO+SN+$H_{0}$+lensing data combination. Left panel: two-dimensional marginalized posterior contours (68.3% and 95.4% CL) in the $m_{\nu,{\rm{sterile}}}^{\rm{eff}}$--$w$ plane. Right panel: two-dimensional marginalized posterior contours (68.3% and 95.4% CL) in the $N_{\rm{eff}}$--$w$ plane.
  • Figure 4: Constraint results for the HDE+$\nu_s$ model from the Planck TT,TE,EE+lowP+BAO data combination and the Planck TT,TE,EE+lowP+BAO+SN+$H_{0}$+lensing data combination. Left panel: two-dimensional marginalized posterior contours (68.3% and 95.4% CL) in the $m_{\nu,{\rm{sterile}}}^{\rm{eff}}$--$c$ plane. Right panel: two-dimensional marginalized posterior contours (68.3% and 95.4% CL) in the $N_{\rm{eff}}$--$c$ plane.
  • Figure 5: The one-dimensional posterior distributions of $H_0$ in the $\Lambda$CDM+$\nu_s$, $w$CDM+$\nu_s$, and HDE+$\nu_s$ models, from the constraints of Planck TT,TE,EE+lowP+BAO ( left) and Planck TT,TE,EE+lowP+BAO+SN+$H_0$+lensing ( right).