The formation of CDM haloes II: collapse time and tides

TL;DR

This study uses cosmological simulations to evaluate and improve the ellipsoidal collapse model for dark matter halo formation, revealing non-linear tidal effects and a stable collapse redshift that refine our understanding of halo evolution.

Contribution

The paper identifies limitations of the classic ellipsoidal collapse model and proposes modifications that better match simulation results, especially regarding collapse timing and density contrasts.

Findings

Ellipsoidal collapse model overestimates halo collapse times.

Tidal forces evolve non-linearly, affecting halo formation.

Halo volume stabilizes at a well-defined redshift after turnaround.

Abstract

We use two cosmological simulations of structure formation in the LambdaCDM scenario to study the evolutionary histories of dark-matter haloes and to characterize the Lagrangian regions from which they form. We focus on haloes identified at redshift z_id=0 and show that the classic ellipsoidal collapse model systematically overestimates their collapse times. If one imposes that halo collapse takes place at z_id, this model requires starting from a significantly lower linear density contrast than what is measured in the simulations at the locations of halo formation. We attempt to explain this discrepancy by testing two key assumptions of the model. First, we show that the tides felt by collapsing haloes due to the surrounding large-scale structure evolve non-linearly. Although this effect becomes increasingly important for low-mass haloes, accounting for it in the ellipsoidal collapse model only marginally improves the agreement with N-body simulations. Second, we track the time evolution of the physical volume occupied by forming haloes and show that, after turnaround, it generally stabilizes at a well-defined redshift, z_c>z_id, contrary to the basic assumption of extended Press-Schechter theory based on excursion sets. We discuss the implications of this result for understanding the origin of the mass-dependence and scatter in the linear threshold for halo formation. Finally, we show that, when tuned for collapse at z_c, a modified version of the ellipsoidal collapse model that also accounts for the triaxial nature of protohaloes predicts their linear density contrast in an unbiased way.