2010
DOI: 10.1063/1.3473861
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A quantum mechanics glimpse to standard cosmology

Abstract: Abstract. In this work we present a connection between a standard cosmology model for inflation and quantum mechanics. We consider a time independent Schrödinger type equation derived from the equations of motion for a single scalar field in a flat space time with a FRW metric and a cosmological constant; the fact that the equation of motion is precisely a Schrödinger equation allows us to investigate on the algebraic relations between the two models and probe the consequences derived from this point of view.

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Cited by 15 publications
(31 citation statements)
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“…[37]. Except the above advantages, the thick branewolrd models also have the following promising features: (1) the effective low energy theory includes a localized massless graviton which can be used to produce the four-dimensional Newtonian potential [26,27,[38][39][40][41][42][43][44][45][46][47][48][49]; (2) the massless scalar graviton decouples from the brane system which avoids the fifth force [38,[50][51][52]; (3) the localization of the fermion field and its chirality can be guaranteed by introducing an interaction with the background scalar field [53][54][55][56]; (4) the gauge field also can be localized on the brane if a mass term is added [57][58][59]; (5) the charge universality of the gauge boson can also be obtained via the Dvali-Shifman mechanism [60][61][62][63][64]. Thus, the thick braneworld model is a kind of candidate model producing both Standard Model and Newtonian gravity, which are two key elements forming our four-dimensional world.…”
Section: Introductionmentioning
confidence: 99%
“…[37]. Except the above advantages, the thick branewolrd models also have the following promising features: (1) the effective low energy theory includes a localized massless graviton which can be used to produce the four-dimensional Newtonian potential [26,27,[38][39][40][41][42][43][44][45][46][47][48][49]; (2) the massless scalar graviton decouples from the brane system which avoids the fifth force [38,[50][51][52]; (3) the localization of the fermion field and its chirality can be guaranteed by introducing an interaction with the background scalar field [53][54][55][56]; (4) the gauge field also can be localized on the brane if a mass term is added [57][58][59]; (5) the charge universality of the gauge boson can also be obtained via the Dvali-Shifman mechanism [60][61][62][63][64]. Thus, the thick braneworld model is a kind of candidate model producing both Standard Model and Newtonian gravity, which are two key elements forming our four-dimensional world.…”
Section: Introductionmentioning
confidence: 99%
“…In this work, we analyse the CE in the pure geometrical thick brane of Reference [29]. A manifold endowed with Weyl structure is considered, wherein Weyl scalar employs the thickness of the brane [29][30][31]. For this reason, the building of these Weyl thick brane models [32][33][34] arise naturally without the necessity of introducing them "by hand".…”
Section: Introductionmentioning
confidence: 99%
“…Usually, in five dimension fermion do not have a normalizable zero mode without scalar-fermion coupling [34]- [42]. In five dimension, with a Yukawa scalar-fermion coupling there may exist a massless bound state and a continuous gapless spectrum of massive Kaluza-Klein (KK) states [38,43], while in some of other brane models, there exist some discrete KK state and a continuous gapless mass spectrum starting from positive m 2 [44,45]. This paper is organized as follows.…”
Section: Introductionmentioning
confidence: 99%