PBH in single field inflation: the effect of shape dispersion and non-Gaussianities

TL;DR

This paper investigates how shape dispersion and non-Gaussianities influence primordial black hole formation in single field inflation, highlighting the dominant formation channels and the importance of non-perturbative effects.

Contribution

It introduces a detailed analysis of non-Gaussianities and shape dispersion effects on PBH formation thresholds, emphasizing the significance of non-perturbative templates.

Findings

For $f_{NL} \,\gtrsim\, 3.5$, false vacuum regions dominate PBH production.

Non-perturbative non-Gaussianity templates are crucial for accurate threshold estimates.

Dispersion effects are minor for the compaction function but relevant at low $f_{NL}$.

Abstract

Primordial black holes (PBHs) may result from high peaks in a random field of cosmological perturbations. In single field inflationary models, such perturbations can be seeded as the inflaton overshoots a small barrier on its way down the potential. PBHs are then produced through two distinct mechanisms, during the radiation era. The first one is the familiar collapse of large adiabatic overdensities. The second one is the collapse induced by relic bubbles where the inflaton field is trapped in a false vacuum, due to large backward fluctuations which prevented horizon sized regions from overshooting the barrier. We consider (numerically and analytically) the effect of non-Gaussianities on the threshold for overdensities to collapse into a PBH. Since typical high peaks have some dispersion in their shape or profile, we also consider the effect of such dispersion on the corresponding threshold for collapse. With these results we estimate the most likely channel for PBH production as a function of the non-Gaussianity parameter $f_{\rm NL}$. We also compare the threshold for collapse coming from the perturbative versus the non perturbative template for the non-Gaussianity arising in this model. We show that i) for $f_{\rm NL}\gtrsim 3.5$, the population of PBH coming from false vacuum regions dominates over that which comes from the collapse of large adiabatic overdensities, ii) the non-perturbative template of the non-Gaussianities is important to get accurate results. iii) the effect of the dispersion is small in determining the threshold for the compaction function, although it can be appreciable in determining the threshold amplitude for the curvature perturbation at low $f_{\rm NL}$. We also confirm that the volume averaged compaction function provides a very accurate universal estimator for the threshold.