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Weighing Neutrinos with Galaxy Surveys

Wayne Hu, Daniel J. Eisenstein, Max Tegmark

Abstract

We show that galaxy redshift surveys sensitively probe the neutrino mass, with eV mass neutrinos suppressing power by a factor of two. The Sloan Digital Sky Survey can potentially detect $N$ nearly degenerate massive neutrino species with mass m_nu > 0.65 (Omega_m h^2/0.1 N)^{0.8} eV at better than 2sigma once microwave background experiments measure two other cosmological parameters. Significant overlap exists between this region and that implied by the LSND experiment, and even m_nu ~ 0.01-0.1 eV, as implied by the atmospheric anomaly, can affect cosmological measurements.

Weighing Neutrinos with Galaxy Surveys

Abstract

We show that galaxy redshift surveys sensitively probe the neutrino mass, with eV mass neutrinos suppressing power by a factor of two. The Sloan Digital Sky Survey can potentially detect nearly degenerate massive neutrino species with mass m_nu > 0.65 (Omega_m h^2/0.1 N)^{0.8} eV at better than 2sigma once microwave background experiments measure two other cosmological parameters. Significant overlap exists between this region and that implied by the LSND experiment, and even m_nu ~ 0.01-0.1 eV, as implied by the atmospheric anomaly, can affect cosmological measurements.

Paper Structure

This paper contains 4 equations, 3 figures.

Figures (3)

  • Figure 1: Effect of a 1 eV neutrino on the BRG power spectrum compared with expected precision of the SDSS BRG survey (1$\sigma$ error boxes, assuming $\sigma_8=2$ for the BRGs). Upper curves: an $\Omega_m=1.0$, $h=0.5$, $\Omega_b h^2=0.0125$, $n=1$ model with and without a 1 eV neutrino mass. Lower curves: the same but for an $\Omega_m=0.2$, $h=0.65$ model.
  • Figure 2: Standard deviation $\sigma({m_\nu})$ as a function of the upper cutoff $k_{\rm max}$ for several different choices of prior cosmological constraints. Models are the same as in Fig. \ref{['fig:neutrino_1']} and have $m_\nu=1{\rm\,eV}$. ( a) High $\Omega_m h^2$: no priors, solid line; single prior of $\sigma(\Omega_m h^2)=0.04$, dashed line; full CMB prior (see text), long-dashed line. ( b) Low $\Omega_m h^2$: as ( a), save that the single prior is $\sigma(n)=0.06$, dashed line.
  • Figure 3: The $2\sigma$ detection threshold for $m_\nu$ from the SDSS BRG survey as a function of the matter density $\Omega_m h^2$ for the number of degenerate mass neutrinos $N=1$--3. We have used $h=0.5$, $\Omega_bh^2=0.0125$, $n=1$, and $k_{\rm max}=0.2h{\rm\,Mpc}^{-1}$; variations on these produce only mild shifts.