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Applicability of the linearly perturbed FRW metric and Newtonian cosmology
Cosmology and Nongalactic Astrophysics · Submitted 25 Feb 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We discuss why the arguments based on the linear theory are not valid.
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The abstract, sentence by sentence
It has been argued that the effect of cosmological structure formation on the average expansion rate is negligible, because the linear approximation to the metric remains applicable in the regime of non-linear density perturbations. We discuss why the arguments based on the linear theory are not valid. We emphasise the difference between Newtonian gravity and the weak field, small velocity limit of general relativity in the cosmological setting.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It has been argued that the effect of cosmological structure formation on the average expansion rate is negligible, because the linear approximation to the metric remains applicable in the regime of non-linear density perturbations. | background 1.00 | 0.04 | 0.08 | asserted 0.91 |
| s1 | We discuss why the arguments based on the linear theory are not valid. | contribution 0.99 | 0.78 | 0.22 | asserted 0.90 |
| s2 | We emphasise the difference between Newtonian gravity and the weak field, small velocity limit of general relativity in the cosmological setting. | contribution 0.95 | 0.71 | 0.11 | asserted 0.77 |
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The paper
Original abstract
It has been argued that the effect of cosmological structure formation on the average expansion rate is negligible, because the linear approximation to the metric remains applicable in the regime of non-linear density perturbations. We discuss why the arguments based on the linear theory are not valid. We emphasise the difference between Newtonian gravity and the weak field, small velocity limit of general relativity in the cosmological setting.
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References
How the literature uses it
18 arXiv papers cite this in 35 sentences
Papers citing it · 31 sentences without a confident label
Cites it as support 1 paper
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However, when density perturbations become nonlinear, contributions from higher order terms become as important as the second order terms [ref] .
Backreaction in late-time cosmology · Perturbative arguments · 0.96
Cites it as background 3 papers
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The second question has been studied in many papers with regard to the average expansion rate [ref] (see [ref] for further discussion and references).
Light propagation and the average expansion rate in near-FRW universes · Introduction · 0.96
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There has been much discussion about the possible gauge-dependence of the average expansion rate [ref] .
Backreaction in late-time cosmology · The average expansion rate · 0.95
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An unresolved issue in cosmology is the effect of the structure formation on the cosmological observations beyond perturbative analysis of the Friedmann-Robertson-Walker or FRW models [ref] .
On the role of shear in cosmological averaging · Introduction · 0.99
What it cites · 151 sentences without a confident label
Contests 10 papers
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However, this is not the case: for a metric of the form metric, the velocity $u^i$ (and thus also $θ$) expanded as a series in $Φ$ necessarily contains an infinite (or zero) number of spatial derivatives [ref] .
Dark energy from backreaction · The perturbative calculation · contest 0.80
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The effect of backreaction cannot be described merely as a change in the FRW background [ref] , unlike argued in [ref] .
Light propagation in statistically homogeneous and isotropic dust universes · The perturbative calculation · contest 0.75
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The effect of backreaction cannot be described merely as a change in the FRW background [ref] , unlike argued in [ref] .
Cosmological background solutions and cosmological backreactions · The perturbative calculation · contest 0.75
Cites as support 16 papers
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Analysis of the Newtonian theory in this case would be misleading, because the Newtonian solutions betray no sign of the fact that starting from general relativity, they do not exist, even at small velocities and weak fields[This underlines that it is not sufficient to look at the Newtonian limit of the equations of general relativity, but it is necessary to consider the limit of solutions, because in general the operations of taking the limit and solving the equations do not commute [ref] .].
Theorems on shear-free perfect fluids with their Newtonian analogues · The Newtonian limit · 0.99
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The variance of the expansion rate and the shear combine to give a total derivative, so $$ reduces to a boundary term [ref] .
Averaging inhomogeneous Newtonian cosmologies · The Newtonian limit · 0.98
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And at second order, the metric cannot be written in the simple diagonal form metric [ref] .
Relativistic second-order perturbations of the Einstein-de Sitter Universe · The perturbative calculation · 0.98
Cites as background 12 papers
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It has been proposed that the observed increase in the expansion rate and the distance scale of the universe at late times relative to the matter-dominated homogeneous and isotropic Friedmann-Robertson-Walker (FRW) model could be explained by the breakdown of the homogeneous and isotropic approximation because of the formation of non-linear structures [ref] .
Accelerated expansion without dark energy · Introduction · 0.80
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It has been proposed that the observed increase in the expansion rate and the distance scale of the universe at late times relative to the matter-dominated homogeneous and isotropic Friedmann-Robertson-Walker (FRW) model could be explained by the breakdown of the homogeneous and isotropic approximation because of the formation of non-linear structures [ref] .
On average properties of inhomogeneous cosmologies · Introduction · 0.80
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It has been proposed that the observed increase in the expansion rate and the distance scale of the universe at late times relative to the matter-dominated homogeneous and isotropic Friedmann-Robertson-Walker (FRW) model could be explained by the breakdown of the homogeneous and isotropic approximation because of the formation of non-linear structures [ref] .
Dark energy from backreaction · Introduction · 0.80
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