2016
DOI: 10.1088/1475-7516/2016/08/015
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On post-inflation validity of perturbation theory in Horndeski scalar-tensor models

Abstract: Abstract. By using the newtonian gauge, we re-confirm that, as in the minimal case, the re-scaled Mukhanov-Sasaki variable is conserved leading to a constraint equation for the Newtonian potential. However, conversely to the minimal case, in Horndeski theories, the super-horizon Newtonian potential can potentially grow to very large values after inflation exit. If that happens, inflationary predictability is lost during the oscillating period. When this does not happen, the perturbations generated during infla… Show more

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Cited by 6 publications
(14 citation statements)
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“…By looking at the Hubble equations (see for example [3]), on an homogeneous and isotropic background one easily find the boundφ 2 < 2 3 M 2 M 2 p . In fact, in average φ2 2 3 M 2 M 2 p [12]. As discussed before, we are interested in the case in which some canonical scalar quanta could spontaneously scatter with up to the background energy.…”
Section: New Higgs Inflationmentioning
confidence: 99%
“…By looking at the Hubble equations (see for example [3]), on an homogeneous and isotropic background one easily find the boundφ 2 < 2 3 M 2 M 2 p . In fact, in average φ2 2 3 M 2 M 2 p [12]. As discussed before, we are interested in the case in which some canonical scalar quanta could spontaneously scatter with up to the background energy.…”
Section: New Higgs Inflationmentioning
confidence: 99%
“…We note that even though the singular behavior atφ = ±φ c disappears at the solution level, one cannot avoid the blow-up of the curvature perturbation ζ k wheṅ φ = 0. This means that ζ is unphysical and thus, one has to reanalyze the perturbation during the reheating by looking for a physical gauge [23]. This is the Newtonian gauge.…”
Section: (418)mentioning
confidence: 99%
“…This is so because the curvature perturbation ζ blows up atφ = 0 on superhorizon scales. We have to re-analyze the perturbations by choosing a different gauge without problems atφ = 0 [23]. To this end, we consider the scalar perturbation around the background (φ = φ(t) + ϕ(t, x)) and the Newtonian gauge [28].…”
Section: Perturbation Analysis In the Newtonian Gaugementioning
confidence: 99%
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