Cosmology and Nongalactic Astrophysics · arXiv:2409.00024 v1 · submitted 16 Aug 2024
Cosmic averaging over multiscaled structure: on foliations, gauges and backreaction
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“In this paper we demonstrate that the implied backreaction terms are artificial, that is gauge dependent, which may easily cause ambiguous estimates of its significance.”
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Abstract
The observation that accelerated cosmic expansion is dominant since the Mega-parsec cosmic structure became nonlinear seems like an extraordinary coincidence, unless the acceleration is somehow driven by the emergence of the structure. That has given rise to the controversial concept of a gravitational backreaction through which inhomogeneity becomes a driver of accelerated expansion. The standard route when studying strongly inhomogeneous cosmological models is to take either a perturbative approach or a spatial averaging approach. Here we argue that because backreaction is in fact a nonlinear multiscale phenomenon, perturbative approaches may have a limited validity. The alternative is the proposed averaging approach. In this paper we demonstrate that the implied backreaction terms are artificial, that is gauge dependent, which may easily cause ambiguous estimates of its significance. In the current study, we forward a formal fully geometric framework of cosmic foliations in the context of relativistic cosmology. Here we show that fixing a foliation of spacetime determines a choice of gauge. Addressing the correspondence between the metric tensor and the foliation allows us to clarify the theoretical implications of choosing a foliation. Within the context of backreaction, this formalism allows us to discuss the complications of averaging. It reveals that spatial averaging can induce artificial backreaction terms that arise from any specific choice of gauge. Averaging methods presented so far all encounter this problem. Within our foliation framework, we can produce a gauge invariant method of averaging by considering a group of proper time foliations which any cosmic observe can agree upon. We demonstrate that this implies the gauge invariance of the averaging procedure. This makes it applicable to standard cosmological simulations.
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abstract compiled · 2026-09-23 · no language-model review
How the main claim is stated: asserted 0.89
What the abstract itself states, as probabilities: claims first 0.07 · states limitation 0.30 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.03 · compares with prior results 0.84 · mentions code or data availability 0.02
The abstract, sentence by sentence
This table labels the abstract only (arXiv listing abstract v1). The number is the probability the classifier gave the label.
| Sentence | Role | The authors' own work | States the main conclusion | Strength |
|---|---|---|---|---|
| The observation that accelerated cosmic expansion is dominant since the Mega-parsec cosmic structure became nonlinear seems like an extraordinary coincidence, unless the acceleration is somehow driven by the emergence of the structure. | background 1.00 | 0.06 | 0.04 | hedged possibility 0.60 |
| That has given rise to the controversial concept of a gravitational backreaction through which inhomogeneity becomes a driver of accelerated expansion. | background 1.00 | 0.03 | 0.03 | asserted 0.90 |
| The standard route when studying strongly inhomogeneous cosmological models is to take either a perturbative approach or a spatial averaging approach. | background 1.00 | 0.04 | 0.02 | asserted 0.99 |
| Here we argue that because backreaction is in fact a nonlinear multiscale phenomenon, perturbative approaches may have a limited validity. | background 0.58 | 0.20 | 0.06 | hedged possibility 0.98 |
| The alternative is the proposed averaging approach. | background 0.68 | 0.07 | 0.04 | asserted 0.82 |
| In this paper we demonstrate that the implied backreaction terms are artificial, that is gauge dependent, which may easily cause ambiguous estimates of its significance. | result 0.95 | 0.61 | 0.51 | asserted 0.89 |
| In the current study, we forward a formal fully geometric framework of cosmic foliations in the context of relativistic cosmology. | contribution 0.93 | 0.84 | 0.05 | asserted 0.99 |
| Here we show that fixing a foliation of spacetime determines a choice of gauge. | result 0.70 | 0.79 | 0.09 | asserted 1.00 |
| Addressing the correspondence between the metric tensor and the foliation allows us to clarify the theoretical implications of choosing a foliation. | contribution 0.48 | 0.77 | 0.06 | asserted 0.71 |
| Within the context of backreaction, this formalism allows us to discuss the complications of averaging. | contribution 0.61 | 0.55 | 0.05 | asserted 0.77 |
| It reveals that spatial averaging can induce artificial backreaction terms that arise from any specific choice of gauge. | result 0.82 | 0.72 | 0.34 | asserted 0.99 |
| Averaging methods presented so far all encounter this problem. | background 0.45 | 0.10 | 0.07 | asserted 1.00 |
| Within our foliation framework, we can produce a gauge invariant method of averaging by considering a group of proper time foliations which any cosmic observe can agree upon. | method 0.53 | 0.90 | 0.28 | asserted 0.71 |
| We demonstrate that this implies the gauge invariance of the averaging procedure. | result 0.63 | 0.92 | 0.24 | asserted 1.00 |
| This makes it applicable to standard cosmological simulations. | interpretation 0.93 | 0.60 | 0.09 | asserted 0.87 |
What kind of paper the classifier reports this is: method or tool 0.54 · evidence from proof or derivation 0.88
What was examined, and what was not
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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 10,614 input tokens.
Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. This record as JSON
How the literature uses it
What this paper does with the arXiv papers it cites
Papers whose main result relates to this one's
States the same result 1 paper
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However, within our foliation framework, we can produce a gauge invariant method of averaging by invoking the gauge-invariant Bardeen formalism for cosmological perturbation theory.
Averaging over cosmic structure: Cosmological backreaction and the gauge problem · 0.86
What it cites · 101 sentences without a confident label
Contests 1 paper
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This also troubles the derivation of $t_μν^(0)$ being a positive energy density is a direct consequence of the backreaction term being traceless, cf. Equation (31) up to (34) of [ref] .
A new framework for analyzing the effects of small scale inhomogeneities in cosmology · Perturbative approach subject to multiscaled structure · contest 0.79
Uses the method or tool of 3 papers
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To overcome this problem, Gasperini et al. [ref] construct and utilize an averaging procedure, [equation] where $S = S ∘ϕ^-1$ and $h = h ∘ϕ^-1$ with $ϕ$ being the map $ϕ(t, x) = (ϕ^1(t,x), x ) = (τ, x)$ such that the foliation are now slices over $ϕ(t, x) =const$.
Gauge invariant averages for the cosmological backreaction · Gauge-invariant averaging: the Gasperini suggestion · 0.88
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To overcome this problem, Gasperini et al. [ref] construct and utilize an averaging procedure, [equation] where $S = S ∘ϕ^-1$ and $h = h ∘ϕ^-1$ with $ϕ$ being the map $ϕ(t, x) = (ϕ^1(t,x), x ) = (τ, x)$ such that the foliation are now slices over $ϕ(t, x) =const$.
A covariant and gauge invariant formulation of the cosmological "backreaction" · Gauge-invariant averaging: the Gasperini suggestion · 0.88
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To overcome this problem, Gasperini et al. [ref] construct and utilize an averaging procedure, [equation] where $S = S ∘ϕ^-1$ and $h = h ∘ϕ^-1$ with $ϕ$ being the map $ϕ(t, x) = (ϕ^1(t,x), x ) = (τ, x)$ such that the foliation are now slices over $ϕ(t, x) =const$.
Light-cone averaging in cosmology: formalism and applications · Gauge-invariant averaging: the Gasperini suggestion · 0.88
Compares with 1 paper
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Relating to literature on the backreaction, we contrast this to the discussion in e.g. Buchert & Räsänen [ref] , where perturbation-gauge transformations $δT ↦δT$, coordinate transformations $x^μ↦x^μ$ and foliation transformation $F ↦F$ (discussed below) are seen as independent constructions.
Backreaction in late-time cosmology · Relativistic cosmology as gauge theory · 0.82
Cites as support 8 papers
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For example, Korzyński [ref] rigorously shows that there are nonlinear effects caused by the way cosmic structure is nested and hierarchically distributed, and that these cannot be included within Newtonian gravity or first-order relativistic perturbation theory.
Nonlinear effects of general relativity from multiscale structure · Averaging approach subject to multiscaled structure · 0.98
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As viewed from these different perspectives, the integral and the corresponding 4-dimensional average is, thus, generally not gauge-invariant, cf. Gasperini et al. [ref] .
Gauge invariant averages for the cosmological backreaction · Foliation gauge transformations over 4-dimensional volumes · 0.99
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And even if suitable backgrounds are identified, the choice of background hugely affects the physical results [ref] , in particular, the backreaction [ref] .
Cosmological Backreaction in Spherical and Plane Symmetric Dust-Filled Space-Times · Perturbative approach subject to multiscaled structure · 0.98
Cites as background 39 papers
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One of the present most prominent perturbative backreaction approaches is that of Green & Wald [ref] .
Examples of backreaction of small scale inhomogeneities in cosmology · Perturbative approach subject to multiscaled structure · 0.89
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One of the present most prominent perturbative backreaction approaches is that of Green & Wald [ref] .
A new framework for analyzing the effects of small scale inhomogeneities in cosmology · Perturbative approach subject to multiscaled structure · 0.89
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One of the present most prominent perturbative backreaction approaches is that of Green & Wald [ref] .
Newtonian and Relativistic Cosmologies · Perturbative approach subject to multiscaled structure · 0.89
Challenges and discussion
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