Identifying the most crucial parameters of the initial curvature profile for primordial black hole formation
T Nakama, T Harada, AG Polnarev… - Journal of Cosmology …, 2014 - iopscience.iop.org
T Nakama, T Harada, AG Polnarev, J Yokoyama
Journal of Cosmology and Astroparticle Physics, 2014•iopscience.iop.orgPrimordial black holes (PBHs) are an important tool in cosmology to probe the primordial
spectrum of small-scale curvature perturbations that reenter the cosmological horizon during
radiation domination epoch. We numerically solve the evolution of spherically symmetric
highly perturbed configurations to clarify the criteria of PBHs formation using an extremely
wide class of curvature profiles characterized by five parameters,(in contrast to only two
parameters used in all previous papers) which specify the curvature profiles not only at the …
spectrum of small-scale curvature perturbations that reenter the cosmological horizon during
radiation domination epoch. We numerically solve the evolution of spherically symmetric
highly perturbed configurations to clarify the criteria of PBHs formation using an extremely
wide class of curvature profiles characterized by five parameters,(in contrast to only two
parameters used in all previous papers) which specify the curvature profiles not only at the …
Abstract
Primordial black holes (PBHs) are an important tool in cosmology to probe the primordial spectrum of small-scale curvature perturbations that reenter the cosmological horizon during radiation domination epoch. We numerically solve the evolution of spherically symmetric highly perturbed configurations to clarify the criteria of PBHs formation using an extremely wide class of curvature profiles characterized by five parameters,(in contrast to only two parameters used in all previous papers) which specify the curvature profiles not only at the central region but also at the outer boundary of configurations. It is shown that formation or non-formation of PBHs is determined essentialy by only two master parameters one of which can be presented as an integral of curvature over initial configurations and the other is presented in terms of the position of the boundary and the edge of the core.
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