Rk. Sheth et B. Jain, THE NONLINEAR CORRELATION-FUNCTION AND DENSITY PROFILES OF VIRIALIZEDHALOES, Monthly Notices of the Royal Astronomical Society, 285(2), 1997, pp. 231-238
The correlation function xi(r) of matter in the non-linear regime is a
ssumed to be determined by the density profiles rho(r) and the mass di
stribution n(M) of virialized haloes. The Press-Schechter approach is
used to compute n(M), and the stable clustering hypothesis is used to
determine the density profiles of these Press-Schechter haloes. Thus,
the shape and amplitude of xi(r) on small scales are related to the in
itial power spectrum of density fluctuations. The case of clustering f
rom scale-free initial conditions is treated in detail. If n is the sl
ope of the initial power spectrum of density fluctuations, then stable
clustering requires that xi(r) proportional to r(-gamma), where gamma
is a known function of n. If halo-halo correlations can be neglected,
then rho(r) proportional to r(-epsilon), where epsilon = (gamma + 3)/
2 = 3(4 + n)/(5 + n). For all values of n of current interest, this sl
ope is steeper than the value 3(3 + n)/(4 + n) that was obtained by Ho
ffman & Shaham in their treatment of the shapes of the outer regions o
f collapsed haloes. Our main result is a prediction for the amplitude
of the non-linear correlation function. The predicted amplitude and it
s dependence on n are in good quantitative agreement with N-body simul
ations of self-similar clustering. If stable clustering is a good appr
oximation only inside the half-mass radii of Press-Schechter haloes, t
hen the density contrast required for the onset of stable clustering c
an be estimated. This density contrast is in the range similar to 300
- 600 and increases with the initial slope n, in agreement with estima
tes from N-body simulations.