2018
DOI: 10.1088/1475-7516/2018/08/048
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The attractive behaviour of ultra-slow-roll inflation

Abstract: It is often claimed that the ultra-slow-roll regime of inflation, where the dynamics of the inflaton field are friction dominated, is a non-attractor and/or transient. In this work we carry out a phase-space analysis of ultra-slow roll in an arbitrary potential, V (φ). We show that while standard slow roll is always a dynamical attractor whenever it is a self-consistent approximation, ultra-slow roll is stable for an inflaton field rolling down a convex potential with M Pl V > |V | (or for a field rolling up a… Show more

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Cited by 70 publications
(70 citation statements)
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“…There has been much work done recently on inflation models with a quasi-inflection point in the potential near the end of inflation. Such a feature introduces a USR period where the inflaton slows down and the necessary amplification of the curvature power spectrum takes place [18,19]. The scales which exit the horizon during this time later re-enter shortly after the end of inflation, whereby the radiation plasma inherits the high curvature perturbation as an increase in the overdensity.…”
Section: Introductionmentioning
confidence: 99%
“…There has been much work done recently on inflation models with a quasi-inflection point in the potential near the end of inflation. Such a feature introduces a USR period where the inflaton slows down and the necessary amplification of the curvature power spectrum takes place [18,19]. The scales which exit the horizon during this time later re-enter shortly after the end of inflation, whereby the radiation plasma inherits the high curvature perturbation as an increase in the overdensity.…”
Section: Introductionmentioning
confidence: 99%
“…Our approach complements the techniques developed in Refs. [16][17][18][19][20][21][22][23][24][25][26][27][28] to study attractor behavior for inflationary models, either by specifying a particular form for the scalar field's potential, V (φ), or by adopting the Hamilton-Jacobi formalism to study the evolution of the Hubble parameter as a function of the scalar field, H(φ).…”
Section: Introductionmentioning
confidence: 99%
“…By varying the Kähler curvature, we can derive the α attractor with n s = 1 − 2/N and r = 12α/N 2 [33], and the α attractor can also be derived from general scalar-tensor theory of gravity [29]. The constant-roll inflation with the slow-roll parameter η H being a constant [34,35] breaks the slow-roll condition if η H is not small and has richer physics than slow-roll inflation because it includes both slow-roll and ultra slow-roll cases [36][37][38][39][40][41][42][43][44][45][46][47][48][49][50][51][52][53][54]. Furthermore, the ultra slow-roll inflation can generate large density perturbation to seed the formation of primordial black holes [55][56][57][58].…”
Section: Introductionmentioning
confidence: 99%