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Brane New World
High Energy Physics - Theory · Submitted 7 Mar 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Since generic matter would be expected to behave like a CFT on small scales, our results suggest that tensor perturbations on small scales are far smaller than predicted by all previous calculations, which have neglected the effects of matter on tensor perturbations.
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The abstract, sentence by sentence
We study a Randall-Sundrum cosmological scenario consisting of a domain wall in anti-de Sitter space with a strongly coupled large $N$ conformal field theory living on the wall. The AdS/CFT correspondence allows a fully quantum mechanical treatment of this CFT, in contrast with the usual treatment of matter fields in inflationary cosmology. The conformal anomaly of the CFT provides an effective tension which leads to a de Sitter geometry for the domain wall. This is the analogue of Starobinsky's four dimensional model of anomaly driven inflation. Studying this model in a Euclidean setting gives a natural choice of boundary conditions at the horizon. We calculate the graviton correlator using the Hartle-Hawking ``No Boundary'' proposal and analytically continue to Lorentzian signature. We find that the CFT strongly suppresses metric perturbations on all but the largest angular scales. This is true independently of how the de Sitter geometry arises, i.e., it is also true for four dimensional Einstein gravity. Since generic matter would be expected to behave like a CFT on small scales, our results suggest that tensor perturbations on small scales are far smaller than predicted by all previous calculations, which have neglected the effects of matter on tensor perturbations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study a Randall-Sundrum cosmological scenario consisting of a domain wall in anti-de Sitter space with a strongly coupled large $N$ conformal field theory living on the wall. | contribution 0.81 | 0.68 | 0.03 | asserted 0.94 |
| s1 | The AdS/CFT correspondence allows a fully quantum mechanical treatment of this CFT, in contrast with the usual treatment of matter fields in inflationary cosmology. | background 0.75 | 0.09 | 0.03 | asserted 1.00 |
| s2 | The conformal anomaly of the CFT provides an effective tension which leads to a de Sitter geometry for the domain wall. | result 0.62 | 0.41 | 0.09 | asserted 1.00 |
| s3 | This is the analogue of Starobinsky's four dimensional model of anomaly driven inflation. | background 0.74 | 0.09 | 0.04 | asserted 1.00 |
| s4 | Studying this model in a Euclidean setting gives a natural choice of boundary conditions at the horizon. | method 0.96 | 0.41 | 0.02 | asserted 0.96 |
| s5 | We calculate the graviton correlator using the Hartle-Hawking ``No Boundary'' proposal and analytically continue to Lorentzian signature. | method 0.99 | 0.94 | 0.03 | asserted 0.99 |
| s6 | We find that the CFT strongly suppresses metric perturbations on all but the largest angular scales. | result 1.00 | 0.96 | 0.53 | asserted 1.00 |
| s7 | This is true independently of how the de Sitter geometry arises, i.e., it is also true for four dimensional Einstein gravity. | interpretation 0.52 | 0.66 | 0.13 | asserted 1.00 |
| s8 | Since generic matter would be expected to behave like a CFT on small scales, our results suggest that tensor perturbations on small scales are far smaller than predicted by all previous calculations, which have neglected the effects of matter on tensor perturbations. | interpretation 1.00 | 0.39 | 0.78 | hedged possibility 1.00 |
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The paper
Original abstract
We study a Randall-Sundrum cosmological scenario consisting of a domain wall in anti-de Sitter space with a strongly coupled large $N$ conformal field theory living on the wall. The AdS/CFT correspondence allows a fully quantum mechanical treatment of this CFT, in contrast with the usual treatment of matter fields in inflationary cosmology. The conformal anomaly of the CFT provides an effective tension which leads to a de Sitter geometry for the domain wall. This is the analogue of Starobinsky's four dimensional model of anomaly driven inflation. Studying this model in a Euclidean setting gives a natural choice of boundary conditions at the horizon. We calculate the graviton correlator using the Hartle-Hawking ``No Boundary'' proposal and analytically continue to Lorentzian signature. We find that the CFT strongly suppresses metric perturbations on all but the largest angular scales. This is true independently of how the de Sitter geometry arises, i.e., it is also true for four dimensional Einstein gravity. Since generic matter would be expected to behave like a CFT on small scales, our results suggest that tensor perturbations on small scales are far smaller than predicted by all previous calculations, which have neglected the effects of matter on tensor perturbations.
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References
How the literature uses it
24 arXiv papers cite this in 35 sentences
Papers citing it · 14 sentences without a confident label
Uses its method or tool 1 paper
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This is the approach chosen in [ref] .
A Tale of Two Hartle-Hawking Wave Functions: Fully Gravitational vs Partially Frozen · Solving for the scalar and vector parts · 0.99
Compares with it 2 papers
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Interestingly, [ref] concluded that the quantum creation of such a universe would be described by the Hartle-Hawking amplitude.
A higher-dimensional view on quantum cosmology · Conclusion · 0.85
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Overall, this reinterpretation of the spacetime geometry seems tantalizingly similar to the situation in Refs. [ref] .
On de Sitter Spacetime and String Theory · The Metric · 0.97
Cites it as background 14 papers
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Due to arguments from the AdS/CFT correspondence [ref] , the low-energy theory on the brane can be described by gravity coupled to a large $N$, strongly coupled CFT [ref] .
Rotating black holes in Randall-Sundrum II braneworlds · Introduction · 0.84
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The duality for RS backgrounds follows the discussions in [ref] and references therein.
Topics in noncommutative integrable theories and holographic brane-world cosmology · Renormalized scalar action · 0.81
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However, there has also been a program, initiated by Hertog and Hartle in [ref] and developed in [ref] , to define the no-boundary wave function more directly in terms of AdS/CFT (earlier ideas in this direction include [ref] ).
Review of the No-Boundary Wave Function · Link to AdS/CFT and Holographic Definition · 0.93
Discussion
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