Published February 15, 2005 | Version v1
Journal article

SDSS galaxy bias from halo mass-bias relation and its cosmological implications

  • 1. Physics Department, Princeton University, Princeton, New Jersey 08544 (United States)
  • 2. Center for Cosmology and Particle Physics, Department of Physics, New York University, 4 Washington Place, New York, New York 10003 (United States)
  • 3. Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 (United States)
  • 4. Department of Physics, University of Pennsylvania, Philadelphia, Pennsylvania 19101 (United States)
  • 5. Princeton University Observatory, Princeton, New Jersey 08544 (United States)
  • 6. Apache Point Observatory, 2001 Apache Point Road, Sunspot, New Mexico 88349-0059 (United States)

Description

We combine the measurements of luminosity dependence of bias with the luminosity dependent weak lensing analysis of dark matter around galaxies to derive the galaxy bias and constrain amplitude of mass fluctuations. We take advantage of theoretical and simulation predictions that predict that, while halo bias is rapidly increasing with mass for high masses, it is nearly constant in low mass halos. We use a new weak lensing analysis around the same Sloan Digital Sky Survey (SDSS) galaxies to determine their halo mass probability distribution. We use these halo mass probability distributions to predict the bias for each luminosity subsample. Galaxies below L* are antibiased with b<1 and for these galaxies bias is only weakly dependent on luminosity. In contrast, for galaxies above L* bias is rapidly increasing with luminosity. These observations are in an excellent agreement with theoretical predictions based on weak lensing halo mass determination combined with halo bias-mass relations. We find that for standard cosmological parameters theoretical predictions are able to explain the observed luminosity dependence of bias over six magnitudes in absolute luminosity. We combine the bias constraints with those from the Wilkinson Microwave Anisotropy Probe (WMAP) and the SDSS power spectrum analysis to derive new constraints on bias and σ8. For the most general parameter space that includes running and neutrino mass, we find σ8=0.88±0.06 and b*=0.99±0.07. In the context of spatially flat models we improve the limit on the neutrino mass for the case of three degenerate families from mν<0.6 eV without bias to mν<0.18 eV with bias (95% C.L.), which is weakened to mν<0.24 eV if running is allowed. The corresponding limit for 3 massless+1 massive neutrino is 1.37 eV

Additional details

Publishing Information

Journal Title
Physical Review. D, Particles Fields
Journal Volume
71
Journal Issue
4
Journal Page Range
p. 043511-043511.18
ISSN
0556-2821
CODEN
PRVDAQ

Optional Information

Notes
(c) 2005 The American Physical Society