2018
DOI: 10.48550/arxiv.1803.02837
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Primordial Black Holes from String Inflation

Michele Cicoli,
Victor A. Diaz,
Francisco G. Pedro
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Cited by 22 publications
(41 citation statements)
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“…For quasi-inflection inflation instead it has been argued [9,13] that the super-horizon growth of R is due to entropy perturbations. Nevertheless, in agreement with the general analysis given in [8], it has also been [14][15][16][17] shown in different scenarios that the super-horizon growth of R can be explained uniquely in terms of the evolution of the background, so it is important to clarify if non adiabatic perturbations actually play any important role.…”
Section: Introductionsupporting
confidence: 73%
“…For quasi-inflection inflation instead it has been argued [9,13] that the super-horizon growth of R is due to entropy perturbations. Nevertheless, in agreement with the general analysis given in [8], it has also been [14][15][16][17] shown in different scenarios that the super-horizon growth of R can be explained uniquely in terms of the evolution of the background, so it is important to clarify if non adiabatic perturbations actually play any important role.…”
Section: Introductionsupporting
confidence: 73%
“…Whilst such a potential can certainly be manufactured within effective field theory, ultimately its shape -and robustness against quantum corrections -would have to be explained within a fundamental theory, like string theory. For example, an attempt towards embedding this model within string theory via fine-tuned string-loop corrections in fibre inflation has been made very recently in [12], although it has not yet proved possible to fine-tune a setup such that cosmological 1 A possible obstacle for PBH's as Dark Matter in this mass range is the constraints arise due to capture of PBH by stars during their formation which may limit the PBH abundance to no more than one percent of the Dark Matter density [6].…”
Section: Introductionmentioning
confidence: 99%
“…All time dependent quantities in the expressions above should be evaluated at the time of horizon crossing11 N hc where the comoving pivot scale k = k * leaves the horizon (a hc H hc ) −1 . To determine the time of horizon crossing, we first use the numerical solutions to the FRW background equations (3.4) to describe the evolution of the Hubble slow-roll parameters in (3.9) in terms of the number of e-folds N and then impose the following measurements and bounds on the CMB observables from12 Planck 2015 (at k * = 0.05 Mpc −1 and 68% CL for TT+lowP+BAO)[47], ln(10 10 A s ) = 3.093 ± 0.034, n s = 0.9673 ± 0.0043, α s = −0.0125 ± 0.0091, r < 0.166 (the Planck/KEK combined analysis gives r < 0.07),(3.11)…”
mentioning
confidence: 99%
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“…In these backgrounds, the amplitude of ζ displays a rapid growth for wavelengths larger than H −1 . This has propelled considerably interest in studying the effects of transient non-attractor periods during inflation as a way of generating primordial black holes (PBHs) [21][22][23][24][25][26][27][28][29][30][31][32][33][34]. For the same reasons, the status of non-Gaussianity in non-attractor models has remained a matter of great interest.…”
mentioning
confidence: 99%