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On Metric Preheating
High Energy Physics - Phenomenology · Submitted 8 Jun 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Employing perturbation theory with backreaction included as spatial averages to second order in the scalar fields and in the metric, we argue that the usual inflationary prediction for metric perturbations on scales relevant for structure formation is not strongly modified.
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The abstract, sentence by sentence
We consider the generation of super-horizon metric fluctuations during an epoch of preheating in the presence of a scalar field \chi quadratically coupled to the inflaton. We find that the requirement of efficient broad resonance is concomitant with a severe damping of super-horizon \delta\chi quantum fluctuations during inflation. Employing perturbation theory with backreaction included as spatial averages to second order in the scalar fields and in the metric, we argue that the usual inflationary prediction for metric perturbations on scales relevant for structure formation is not strongly modified.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider the generation of super-horizon metric fluctuations during an epoch of preheating in the presence of a scalar field \chi quadratically coupled to the inflaton. | contribution 0.80 | 0.57 | 0.05 | unclear 0.48 |
| s1 | We find that the requirement of efficient broad resonance is concomitant with a severe damping of super-horizon \delta\chi quantum fluctuations during inflation. | result 1.00 | 0.92 | 0.11 | asserted 1.00 |
| s2 | Employing perturbation theory with backreaction included as spatial averages to second order in the scalar fields and in the metric, we argue that the usual inflationary prediction for metric perturbations on scales relevant for structure formation is not strongly modified. | result 0.87 | 0.87 | 0.81 | asserted 0.51 |
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The paper
Original abstract
We consider the generation of super-horizon metric fluctuations during an epoch of preheating in the presence of a scalar field \chi quadratically coupled to the inflaton. We find that the requirement of efficient broad resonance is concomitant with a severe damping of super-horizon \delta\chi quantum fluctuations during inflation. Employing perturbation theory with backreaction included as spatial averages to second order in the scalar fields and in the metric, we argue that the usual inflationary prediction for metric perturbations on scales relevant for structure formation is not strongly modified.
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References
How the literature uses it
8 arXiv papers cite this in 9 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We estimate analytically the upper limit of the amplitude of the metric perturbations for all scales in the limit of so-called broad resonance, and show that the large scale metric perturbations are very small, and taking them into account does not influence the standard picture of the production of the metric perturbations in inflationary scenario.
On generation of metric perturbations during preheating · 0.89
Papers citing it · 7 sentences without a confident label
Cites it as background 2 papers
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This effect of the resonant amplification of the metric perturbations is often quoted as “metric preheating" [ref] .
Studying Aspects of the Early Universe with Primordial Black Holes · The perturbations: The case of metric preheating · 0.83
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These enhanced quantum fluctuations are accompanied by a resonant amplification of the scalar metric fluctuations (usually quoted as metric preheating [ref] ), or, in other terms, with enhanced curvature perturbations, responsible for the generation of SIGWs [ref] and potentially for PBH formation [ref] (see however [ref] for an assessment on the role of non-linearities and anharmonicities).
Reconstructing Primordial Curvature Perturbations via Scalar-Induced Gravitational Waves with LISA · Other classes of models · 0.83
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