4.6 Article

Mass function and bias of dark matter halos for non-Gaussian initial conditions

Journal

ASTRONOMY & ASTROPHYSICS
Volume 514, Issue -, Pages -

Publisher

EDP SCIENCES S A
DOI: 10.1051/0004-6361/200912636

Keywords

gravitation; methods: analytical; large-scale structure of Universe

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Aims. We revisit the derivation of the mass function and the bias of dark matter halos for non-Gaussian initial conditions. Methods. We use a steepest-descent approach to point out that exact results can be obtained for the high-mass tail of the halo mass function and the two-point correlation of massive halos. Focusing on primordial non-Gaussianity of the local type, we check that these results agree with numerical simulations. Results. The high-mass cutoff of the halo mass function takes the same form as the one obtained from the Press-Schechter formalism, but with a linear threshold delta(L) that depends on the definition of the halo (i.e. delta(L) similar or equal to 1.59 for a nonlinear density contrast of 200). We show that a simple formula, which obeys this high-mass asymptotic and uses the fit obtained for Gaussian initial conditions, matches numerical simulations while keeping the mass function normalized to unity. Next, by deriving the real-space halo two-point correlation in the spirit of Kaiser (1984, ApJ, 284, L9) and taking a Fourier transform, we obtain good agreement with simulations for the correction to the halo bias, Delta b(M)(k, f(NL)), due to primordial non-Gaussianity. Therefore, neither the halo mass function nor the bias require an ad-hoc parameter q (such as delta(c) -> delta c root q), provided one uses the correct linear threshold delta(L) and pays attention to halo displacements. The nonlinear real-space expression can be useful for checking that the linearized bias is a valid approximation. Moreover, it clearly shows how the baryon acoustic oscillation at similar to 100h(-1) Mpc is amplified by the bias of massive halos and modified by primordial non-Gaussianity. On smaller scales, 30 < x < 90 h(-1) Mpc, the correction to the real-space bias roughly scales as f(NL) b(M)(f(NL) = 0) x(2). The low-k behavior of the halo bias does not imply a divergent real-space correlation, so that one does not need to introduce counterterms that depend on the survey size.

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