Abstract

We investigate the error implied by the use of the Zel'dovich approximation to set up the initial conditions at a finite redshift z i in numerical simulations. Using a steepest-descent method developed in a previous work (Valageas [CITE]) we derive the probability distribution ${\cal P}(\delta_{R})$ of the density contrast in the quasi-linear regime. This also provides its dependence on the redshift z i at which the simulation is started. Thus, we find that the discrepancy with the exact pdf (defined by the limit $z_{\rm i}\rightarrow \infty$) is negligible after the scale factor has grown by a factor $a/a_{\rm i}\ga 5$, for scales which were initially within the linear regime with $\sigma_{\rm i} \la 0.1$. This shows that the use of the Zel'dovich approximation to implement the initial conditions is sufficient for practical purposes since these are not very severe constraints.

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