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Topics in noncommutative integrable theories and holographic brane-world cosmology
High Energy Physics - Theory · Submitted 7 Dec 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The 7D RS set-up with brane-bulk energy exchange we propose leads to a non conventional cosmological evolution where all fixed points have positive acceleration and are found to be stable for a wide range of choices for the parameters.
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This thesis follows two main lines of research, both related to relevant aspects of string theory and its phenomenological/cosmological applications. We study two different generalizations of the integrable SG model to NC geometry, after discussing general properties and issues of integrable theories and NC field theories, mentioning their role in string theory. The question is whether we can obtain an integrable NC SG with factorized S matrix. Of the two models we study, the second NC SG -- derived by dimensional reduction from the stringy NC self-dual YM in (2+2) dimensions -- exhibits the good properties of S matrix required by integrability in 2D, while the first one does not. As a second topic, a particular brane-world model is analyzed both from the cosmological point of view and in the spirit of holography, after introducing conventional cosmology, brane-worlds and AdS/CFT. The 7D RS set-up with brane-bulk energy exchange we propose leads to a non conventional cosmological evolution where all fixed points have positive acceleration and are found to be stable for a wide range of choices for the parameters. We construct the holographic dual theory, represented by a renormalized 6D CFT coupled to 6D gravity. The matching of parameters on the two sides of the duality is then achieved in specific approximations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | This thesis follows two main lines of research, both related to relevant aspects of string theory and its phenomenological/cosmological applications. | background 0.59 | 0.47 | 0.03 | asserted 0.97 |
| s1 | We study two different generalizations of the integrable SG model to NC geometry, after discussing general properties and issues of integrable theories and NC field theories, mentioning their role in string theory. | contribution 0.99 | 0.87 | 0.04 | asserted 0.96 |
| s2 | The question is whether we can obtain an integrable NC SG with factorized S matrix. | gap 0.70 | 0.12 | 0.03 | unclear 0.53 |
| s3 | Of the two models we study, the second NC SG -- derived by dimensional reduction from the stringy NC self-dual YM in (2+2) dimensions -- exhibits the good properties of S matrix required by integrability in 2D, while the first one does not. | result 1.00 | 0.94 | 0.26 | asserted 1.00 |
| s4 | As a second topic, a particular brane-world model is analyzed both from the cosmological point of view and in the spirit of holography, after introducing conventional cosmology, brane-worlds and AdS/CFT. | contribution 0.87 | 0.76 | 0.03 | asserted 0.95 |
| s5 | The 7D RS set-up with brane-bulk energy exchange we propose leads to a non conventional cosmological evolution where all fixed points have positive acceleration and are found to be stable for a wide range of choices for the parameters. | result 0.98 | 0.94 | 0.27 | asserted 1.00 |
| s6 | We construct the holographic dual theory, represented by a renormalized 6D CFT coupled to 6D gravity. | contribution 0.78 | 0.93 | 0.07 | asserted 1.00 |
| s7 | The matching of parameters on the two sides of the duality is then achieved in specific approximations. | method 0.46 | 0.89 | 0.07 | asserted 1.00 |
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The paper
Original abstract
This thesis follows two main lines of research, both related to relevant aspects of string theory and its phenomenological/cosmological applications. We study two different generalizations of the integrable SG model to NC geometry, after discussing general properties and issues of integrable theories and NC field theories, mentioning their role in string theory. The question is whether we can obtain an integrable NC SG with factorized S matrix. Of the two models we study, the second NC SG -- derived by dimensional reduction from the stringy NC self-dual YM in (2+2) dimensions -- exhibits the good properties of S matrix required by integrability in 2D, while the first one does not. As a second topic, a particular brane-world model is analyzed both from the cosmological point of view and in the spirit of holography, after introducing conventional cosmology, brane-worlds and AdS/CFT. The 7D RS set-up with brane-bulk energy exchange we propose leads to a non conventional cosmological evolution where all fixed points have positive acceleration and are found to be stable for a wide range of choices for the parameters. We construct the holographic dual theory, represented by a renormalized 6D CFT coupled to 6D gravity. The matching of parameters on the two sides of the duality is then achieved in specific approximations.
Human review
How the literature uses it
3 arXiv papers cite this in 3 sentences
Papers citing it
Cites it as background 3 papers
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(For reviews, see e.g. [ref] .) These equations imply no gauge field and noncommutative extension of them perhaps might have no physical picture or no good property on integrability.
Noncommutative Integrable Systems and Quasideterminants · Towards noncommutative integrable systems · 0.95
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(For reviews, see [ref] .) This is partially motivated by recent developments of noncommutative gauge theories on D-branes.
Noncommutative Solitons and Quasideterminants · Introduction · 1.00
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For surveys on integrable systems in noncommutative space-times, see e.g. [ref] .
Soliton Scattering in Noncommutative Spaces · Introduction · 1.00
What it cites · 99 sentences without a confident label
Builds on 1 paper
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So, I now wish to establish the correspondence between this energy exchange and its dual object in the generalization of the holographic theory, following [ref] .
Holography and Brane-bulk Energy Exchange · Holographic cosmology in four dimensions · 0.87
Uses the method or tool of 3 papers
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In this section, I will explain how to construct this renormalized supergravity action following the holographic renormalization procedure [ref] .
Holographic Reconstruction of Spacetime and Renormalization in the AdS/CFT Correspondence · About the (0,2) SCFT in six dimensions · 0.98
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In this section, I will explain how to construct this renormalized supergravity action following the holographic renormalization procedure [ref] .
The Holographic Weyl anomaly · About the (0,2) SCFT in six dimensions · 0.98
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In this section, I will explain how to construct this renormalized supergravity action following the holographic renormalization procedure [ref] .
Quantum effective action from the AdS/CFT correspondence · About the (0,2) SCFT in six dimensions · 0.98
Compares with 3 papers
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Namely, following [ref] one comes to the traces A_(2) = ℓ/16G_N^(3)R A_(4) = ℓ^3/2G_N^(5)(E_(4)+I_(4)) with E_(4) = 1/64(R^ρR_ρ-4r^R_+R^2) I_(4) = -64(R^ρR_ρ-2R^R_+3R^3) being the Euler density and the local conformal invariant in four dimensions.
Holographic Reconstruction of Spacetime and Renormalization in the AdS/CFT Correspondence · Conformal anomaly via holography · 0.90
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Namely, following [ref] one comes to the traces A_(2) = ℓ/16G_N^(3)R A_(4) = ℓ^3/2G_N^(5)(E_(4)+I_(4)) with E_(4) = 1/64(R^ρR_ρ-4r^R_+R^2) I_(4) = -64(R^ρR_ρ-2R^R_+3R^3) being the Euler density and the local conformal invariant in four dimensions.
The Holographic Weyl anomaly · Conformal anomaly via holography · 0.90
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Namely, following [ref] one comes to the traces A_(2) = ℓ/16G_N^(3)R A_(4) = ℓ^3/2G_N^(5)(E_(4)+I_(4)) with E_(4) = 1/64(R^ρR_ρ-4r^R_+R^2) I_(4) = -64(R^ρR_ρ-2R^R_+3R^3) being the Euler density and the local conformal invariant in four dimensions.
Quantum effective action from the AdS/CFT correspondence · Conformal anomaly via holography · 0.90
Cites as background 60 papers
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Let me now introduce the two Randall–Sundrum (RS) models [ref] and the cosmologies that develop specially in the one brane RS set–up.
A Large Mass Hierarchy from a Small Extra Dimension · The Randall–Sundrum alternative · 0.97
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In the model inspired by the Horawa–Witten M theory solution [ref] and proposed by Binétruy, Deffayet and Langlois [ref] the fifth dimension is compactified on a circle which is then orbifolded as in RSI model.
Eleven-Dimensional Supergravity on a Manifold with Boundary · Flat extra dimensions · 0.89
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In the model inspired by the Horawa–Witten M theory solution [ref] and proposed by Binétruy, Deffayet and Langlois [ref] the fifth dimension is compactified on a circle which is then orbifolded as in RSI model.
Non-conventional cosmology from a brane-universe · Flat extra dimensions · 0.89
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