2021
DOI: 10.48550/arxiv.2110.05982
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Primordial black hole formation for an anisotropic perfect fluid: initial conditions and estimation of the threshold

Ilia Musco,
Theodoros Papanikolaou
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Cited by 4 publications
(4 citation statements)
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“…In this paper, we focus on the PBH formation in a nonspherical setting and possible generation of the black hole spin. Although spherically symmetric dynamics for PBH formation has been mainly considered [30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49] for many years, we can also find several works in which nonspherical PBH formation is considered [50][51][52][53][54][55][56][57][58][59]. Some of them [50,51,53] focus on the PBH formation in a matter-dominated universe, in which the non-spherical collapse would be essential for understanding the criterion of the PBH formation.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we focus on the PBH formation in a nonspherical setting and possible generation of the black hole spin. Although spherically symmetric dynamics for PBH formation has been mainly considered [30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49] for many years, we can also find several works in which nonspherical PBH formation is considered [50][51][52][53][54][55][56][57][58][59]. Some of them [50,51,53] focus on the PBH formation in a matter-dominated universe, in which the non-spherical collapse would be essential for understanding the criterion of the PBH formation.…”
Section: Introductionmentioning
confidence: 99%
“…With regards to the PBH formation threshold value, δ c , the latter will depend, in general, on the shape of the collapsing curvature perturbation profile [89,90], on the EoS parameter at the time of PBH formation [91][92][93], as well on the presence of anisotropies [94] and nonsphericities [95,96]. In our case, we consider the standard case of spherical isotropic collapse in the HBB RD expanding era.…”
Section: Jcap06(2024)066mentioning
confidence: 99%
“…As modes are stretched on super-horizon scales during inflation, curvature perturbations freeze-out until they re-enter the horizon during the post-inflationary epoch. At this point, if the amplitude of perturbations is larger than the threshold [44][45][46][47][48][49][50][51], they can collapse forming a population of PBHs with masses controlled by the energy contained in a Hubble volume. Various observations already constrain the fraction of DM composed of PBHs (usually denoted f PBH ≡ Ω PBH /Ω DM ).…”
Section: Introductionmentioning
confidence: 99%