Abstract
We consider black holes which form from an initially spherically symmetric super-Hubble perturbation of a cosmological background filled by a perfect fluid with . Previous work has shown that when (radiation), there is a critical threshold for black hole formation (), which, to a very good approximation, only depends upon the curvature of the compaction function around its peak value. We find that this generalizes to all ; for smaller s the knowledge of the full shape of the compaction function is necessary. We provide analytic approximations for which are accurate for .
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