The power spectrum, bias evolution, and the spatial three-point correlation function

Citation
A. Buchalter et M. Kamionkowski, The power spectrum, bias evolution, and the spatial three-point correlation function, ASTROPHYS J, 521(1), 1999, pp. 1-16
Citations number
72
Categorie Soggetti
Space Sciences
Journal title
ASTROPHYSICAL JOURNAL
ISSN journal
0004637X → ACNP
Volume
521
Issue
1
Year of publication
1999
Part
1
Pages
1 - 16
Database
ISI
SICI code
0004-637X(19990810)521:1<1:TPSBEA>2.0.ZU;2-U
Abstract
We calculate perturbatively the normalized spatial skewness, S-3, and full three-point correlation function (3PCF), zeta, induced by gravitational ins tability of Gaussian primordial fluctuations for a biased tracer-mass distr ibution in flat and open cold dark matter (CDM) models. We take into accoun t the explicit dependence on cosmological parameters, the shape and evoluti on of the CDM power spectrum, and we allow the bias to be nonlinear and/or evolving in time, using an extension of Fry's bias evolution model. We deri ve a scale-dependent, leading-order correction to the standard perturbative expression for S-3 in the case of nonlinear biasing, as defined for the un smoothed galaxy and dark-matter fields, and find that this correction becom es large when probing positive effective power-spectrum indices, i.e., scal es above 100 h(-1) Mpc for reasonable CDM models. This term implies that th e inferred nonlinear-bias parameter, as usually defined in terms of the smo othed density fields, might in general depend on the chosen smoothing scale and could allow better constraints on both the linear- and nonlinear-bias parameters on the basis of skewness measurements alone (or at least disting uish between the smoothed and unsmoothed bias pictures), if S-3 could be me asured over very large scales. In general, we find that the dependence of S -3 on the biasing scheme can substantially outweigh that on the adopted cos mology, with linear and nonlinear bias separately giving rise to distinct s ignatures in the skewness, but degenerate ones in combination. We demonstra te that the normalized 3PCF, Q(v) is an ill-behaved quantity, and speculate that reported discrepancies between perturbative and N-body predictions fo r Q may arise in part from systematic errors associated with the poor choic e of normalization. To avoid this problem we investigate Q(v), the variance -normalized 3PCF. The configuration dependence of Q(v) shows similarly stro ng sensitivities to the bias scheme as S-3, but also exhibits significant d ependence on the form of the CDM power spectrum. Though the degeneracy of S -3 with respect to the cosmological parameters and constant linear- and non linear-bias parameters can be broken by the full configuration dependence o f Q(v), neither statistic can distinguish well between evolving and nonevol ving bias scenarios, since an evolving bias is found to effectively mimic a smaller but constant bias. We show that this can be resolved, in principle , by considering the redshift dependence of zeta, which can also yield dire ct constraints on Ohm(0), and the epoch of galaxy formation.