The formation of CDM haloes I: Collapse thresholds and the ellipsoidal collapse model
arXiv:1107.5808 · doi:10.1093/mnras/stu2021
Abstract
In the excursion set approach to structure formation initially spherical regions of the linear density field collapse to form haloes of mass at redshift if their linearly extrapolated density contrast, averaged on that scale, exceeds some critical threshold, . The value of is often calculated from the spherical or ellipsoidal collapse model, which provide well-defined predictions given auxiliary properties of the tidal field at a given location. We use two cosmological simulations of structure growth in a cold dark matter scenario to quantify , its dependence on the surrounding tidal field, as well as on the shapes of the Lagrangian regions that collapse to form haloes at . Our results indicate that the ellipsoidal collapse model provides an accurate description of the mean dependence of on both the strength of the tidal field and on halo mass. However, for a given , depends strongly on the halo's characteristic formation redshift: the earlier a halo forms, the higher its initial density contrast. Surprisingly, the majority of haloes forming fall below the ellipsoidal collapse barrier, contradicting the model predictions. We trace the origin of this effect to the non-spherical shapes of Lagrangian haloes, which arise naturally due to the asymmetry of the linear tidal field. We show that a modified collapse model, that accounts for the triaxial shape of protohaloes, provides a more accurate description of the measured minimum overdensities of recently collapsed objects.
MNRAS in press
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