2004
DOI: 10.1103/physrevd.70.046005
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Spontaneous decompactification

Abstract: Positive vacuum energy together with extra dimensions of space imply that our fourdimensional Universe is unstable, generically to decompactification of the extra dimensions. Either quantum tunneling or thermal fluctuations carry one past a barrier into the decompactifying regime. We give an overview of this process, and examine the subsequent expansion into the higher-dimensional geometry. This is governed by certain fixed-point solutions of the evolution equations, which are studied for both positive and neg… Show more

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Cited by 49 publications
(74 citation statements)
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“…To be concrete, let us first focus on the case when the three-dimensional cosmological constant is zero and the axion fluxes are absent, so that the effective potential U goes to zero at large values of R. Let us start with the simplest case, when the lower dimensional vacuum has a negative cosmological constant. According to (13) this implies that the effective potential has a maximum at R = R 0 , see Fig. 5.…”
Section: Setting Up the Problem In The Three-dimensional Casementioning
confidence: 99%
“…To be concrete, let us first focus on the case when the three-dimensional cosmological constant is zero and the axion fluxes are absent, so that the effective potential U goes to zero at large values of R. Let us start with the simplest case, when the lower dimensional vacuum has a negative cosmological constant. According to (13) this implies that the effective potential has a maximum at R = R 0 , see Fig. 5.…”
Section: Setting Up the Problem In The Three-dimensional Casementioning
confidence: 99%
“…The scalar potential for the Kähler moduli always goes to zero at infinite volume, and so any minima we might find will be unstable to spontaneous decompactification [75] to ten non-compact dimensions. This is mediated by the same CDL instantons discussed in Sec.…”
Section: Eternal Inflation and The Landscapementioning
confidence: 99%
“…We can also check that our potential (5.8) gives familiar dynamics for the radial dilaton, as described for example in [36,37], as well as better understanding the relation to the alternate expression (5.11). Consider the simpler case where we perturb an unwarped background by a stress tensor due to branes, fluxes, or other sources.…”
Section: Simple Examplesmentioning
confidence: 99%