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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 (zs= 0.1 to 3.6) and on angular scales of θ= 2 to 32 arcmin. In addition, the data have been validated by analytical computations for an identical cosmology, with density parameter Ωm= 0.3 and...

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Published in:Monthly notices of the Royal Astronomical Society 2002-10, Vol.335 (4), p.909-917
Main Author: Barber, Andrew J.
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Language:English
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description The weak lensing shear signal has been measured numerically in N-body simulations at 14 different redshifts (zs= 0.1 to 3.6) and on angular scales of θ= 2 to 32 arcmin. In addition, the data have been validated by analytical computations for an identical cosmology, with density parameter Ωm= 0.3 and vacuum energy density parameter λ0= 0.7. This paper reports on the scale and redshift dependence of the shear variance, 〈γ2〉, which may be described by a simple formula of the form 〈γ2〉 (θ, zs) =a(θ) zsb(θ). The redshift dependence for source redshifts up to 1.6 is found to be close to zs2, which is a stronger dependence than earlier analytical predictions (〈γ2〉∝zs1.52), although, at higher redshifts, the zs 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.
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subjects galaxies: clusters: general
galaxies: distances and redshifts
gravitational lensing
large-scale structure of Universe
methods: N-body simulations
methods: numerical
title The redshift and scale dependence of the cosmic shear signal from numerical simulations
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