RECORD
Evolution of Cosmological Perturbations in the Brane World
High Energy Physics - Theory · Submitted 25 May 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Using our formalism, the late time evolution of the cosmological scalar perturbations at any scales larger than the AdS curvature scale $l$ is shown to be identical with the one obtained in the conventional 4D cosmology, provided the effect of heavy graviton modes may be neglected.
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
The evolution of the cosmological perturbations is studied in the context of the Randall-Sundrum brane world scenario, in which our universe is realized on a three-brane in the five dimensional Anti-de Sitter(AdS) spacetime. We develop a formalism to solve the coupled dynamics of the cosmological perturbations in the brane world and the gravitational wave in the AdS bulk. Using our formalism, the late time evolution of the cosmological scalar perturbations at any scales larger than the AdS curvature scale $l$ is shown to be identical with the one obtained in the conventional 4D cosmology, provided the effect of heavy graviton modes may be neglected. Here the late time means the epoch when the Hubble horizon $H^{-1}$ in the 4D brane world is sufficiently larger than the AdS curvature scale $l$. If the inflation occurs sufficiently lower than $l^{-1}$, the scalar temperature anisotropies in the Cosmic Microwave Background at large scales can be calculated using the constancy of the Bardeen parameter as is done in the 4D cosmology. The assumption of the result is that the effect of the massive graviton with mass $m e^{-\alpha_0}>l^{-1}$ in the brane world is negligible, where $e^{\alpha_0}$ is the scale factor of the brane world. We also discuss the effect of these massive gravitons on the evolution of the perturbations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The evolution of the cosmological perturbations is studied in the context of the Randall-Sundrum brane world scenario, in which our universe is realized on a three-brane in the five dimensional Anti-de Sitter(AdS) spacetime. | background 0.83 | 0.42 | 0.04 | asserted 0.91 |
| s1 | We develop a formalism to solve the coupled dynamics of the cosmological perturbations in the brane world and the gravitational wave in the AdS bulk. | method 0.59 | 0.95 | 0.04 | asserted 0.98 |
| s2 | Using our formalism, the late time evolution of the cosmological scalar perturbations at any scales larger than the AdS curvature scale $l$ is shown to be identical with the one obtained in the conventional 4D cosmology, provided the effect of heavy graviton modes may be neglected. | result 1.00 | 0.92 | 0.81 | asserted 0.99 |
| s3 | Here the late time means the epoch when the Hubble horizon $H^{-1}$ in the 4D brane world is sufficiently larger than the AdS curvature scale $l$. | interpretation 0.87 | 0.29 | 0.04 | asserted 0.93 |
| s4 | If the inflation occurs sufficiently lower than $l^{-1}$, the scalar temperature anisotropies in the Cosmic Microwave Background at large scales can be calculated using the constancy of the Bardeen parameter as is done in the 4D cosmology. | interpretation 0.67 | 0.47 | 0.09 | asserted 0.50 |
| s5 | The assumption of the result is that the effect of the massive graviton with mass $m e^{-\alpha_0}>l^{-1}$ in the brane world is negligible, where $e^{\alpha_0}$ is the scale factor of the brane world. | limitation 0.99 | 0.50 | 0.10 | asserted 0.93 |
| s6 | We also discuss the effect of these massive gravitons on the evolution of the perturbations. | contribution 0.98 | 0.81 | 0.03 | unclear 0.88 |
What was examined, and what was not
- arXiv listing abstract v6
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
The evolution of the cosmological perturbations is studied in the context of the Randall-Sundrum brane world scenario, in which our universe is realized on a three-brane in the five dimensional Anti-de Sitter(AdS) spacetime. We develop a formalism to solve the coupled dynamics of the cosmological perturbations in the brane world and the gravitational wave in the AdS bulk. Using our formalism, the late time evolution of the cosmological scalar perturbations at any scales larger than the AdS curvature scale $l$ is shown to be identical with the one obtained in the conventional 4D cosmology, provided the effect of heavy graviton modes may be neglected. Here the late time means the epoch when the Hubble horizon $H^{-1}$ in the 4D brane world is sufficiently larger than the AdS curvature scale $l$. If the inflation occurs sufficiently lower than $l^{-1}$, the scalar temperature anisotropies in the Cosmic Microwave Background at large scales can be calculated using the constancy of the Bardeen parameter as is done in the 4D cosmology. The assumption of the result is that the effect of the massive graviton with mass $m e^{-\alpha_0}>l^{-1}$ in the brane world is negligible, where $e^{\alpha_0}$ is the scale factor of the brane world. We also discuss the effect of these massive gravitons on the evolution of the perturbations.
Human review
References
How the literature uses it
4 arXiv papers cite this in 4 sentences
Papers whose main result relates to this one's
States the same result 1 paper
-
We show that the behavior of cosmological perturbations on superhorizon scales in the brane-world model is the same as that in the standard no-extradimension model, irrespective of the initial condition for bulk perturbations, in the late stage when the cosmic expansion rate $H$ is smaller than the inverse of the bulk curvature scale $\ell$.
Behavior of Cosmological Perturbations in the Brane-World Mode · 0.93
Papers citing it · 1 sentence without a confident label
Cites it as support 1 paper
-
Since the model we are considering doesn't originate from an exact bulk solution, but rather from a reasonable ansatz for the bulk matter content, a perturbative treatment cannot be particularly helpful. * It turns out that at late times, when the Hubble radius is much greater than the bulk radius of curvature, the results of perturbations appear to be equivalent to those obtained when treating a conventional 4D cosmology [ref] .
Cosmic Acceleration Data and Bulk-Brane Energy Exchange · Introduction · 0.96
Cites it as background 2 papers
-
Cosmological perturbation theory in braneworld cosmology also has some distinct features [ref] .
Density perturbations in braneworld cosmology and primordial black holes · Introduction · 0.95
-
The theory of gauge-invariant perturbations in brane-world cosmology has been extensively investigated and developed [ref] and is qualitatively well understood.
Brane-World Gravity · Brane-World Cosmology: Perturbations · 0.91
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.