2016
DOI: 10.1155/2016/6705021
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Time-Dependent Toroidal Compactification Proposals and the Bianchi Type I Model: Classical and Quantum Solutions

Abstract: We construct an effective four-dimensional model by compactifying a ten-dimensional theory of gravity coupled with a real scalar dilaton field on a time-dependent torus. This approach is applied to anisotropic cosmological Bianchi type I model for which we study the classical coupling of the anisotropic scale factors with the two real scalar moduli produced by the compactification process. Under this approach, we present an isotropization mechanism for the Bianchi I cosmological model through the analysis of t… Show more

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Cited by 1 publication
(5 citation statements)
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“…On the other hand, we see that the solution associated to the equation (41b) is the same for all Bianchi Class A cosmological models. It was the main result obtained in [2,3]. This can be appreciated by observing the Hamiltonian operator (30), which can be split as Ĥ(a, c, φ, σ)Ψ = Ĥg (a, c)Ψ + Ĥm (φ, σ)Ψ = 0, where Ĥg y Ĥm represents the With the last results, we obtain the general solution to the WDW equation ( 40) whose wave function Φ can be built by taking the superposition of the functions (44) and (45), that is…”
Section: Quantum Schemementioning
confidence: 75%
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“…On the other hand, we see that the solution associated to the equation (41b) is the same for all Bianchi Class A cosmological models. It was the main result obtained in [2,3]. This can be appreciated by observing the Hamiltonian operator (30), which can be split as Ĥ(a, c, φ, σ)Ψ = Ĥg (a, c)Ψ + Ĥm (φ, σ)Ψ = 0, where Ĥg y Ĥm represents the With the last results, we obtain the general solution to the WDW equation ( 40) whose wave function Φ can be built by taking the superposition of the functions (44) and (45), that is…”
Section: Quantum Schemementioning
confidence: 75%
“…It was the main result obtained in [3,4]. This can be appreciated by observing the Hamiltonian operator (35), which can be split asĤ(a, c, , )Ψ =Ĥ g (a, c)Ψ + H m ( , )Ψ = 0, whereĤ g yĤ m represents the Hamiltonian for gravitational sector and the moduli fields, respectively, and the scale factors have the transformations = , = .…”
Section: − 16 11mentioning
confidence: 86%
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