The redshift and scale dependence of the cosmic shear signal from numerical simulations

The weak lensing shear signal has been measured numerically in N-body simulations at 14 different redshifts (z(s) = 0.1 to 3.6) and on angular scales of theta = 2 to 32 arcmin. In addition, the data have been validated by analytical computations for an identical cosmology, with density parameter Omega(m) = 0.3 and vacuum energy density parameter lambda(0) = 0.7. This paper reports on the scale and redshift dependence of the shear variance, [gamma(2)], which may be described by a simple formula of the form [gamma(2)] (theta, z(s)) = a (theta) z(s)(b(theta)). The redshift dependence for source redshifts up to 1.6 is found to be close to z(s)(2), which is a stronger dependence than earlier analytical predictions ([gamma(2)] proportional to z(s)(1.52)), although, at higher redshifts, the z(s) dependence of the shear variance is clearly less steep. The strong redshift dependence further emphasizes the need to know the precise redshift distribution for the galaxy sources in any given survey, so that they can be allocated to redshift bins accordingly, and the cosmic shear signal correctly interpreted. Equations are also given for the variance in the reduced shear, which is a more directly measurable quantity observationally.