Modeling the fifth dimension with scalars and gravity

TL;DR

This paper develops a first-order differential equation method inspired by gauged supergravity to find solutions in five-dimensional scalar-gravity models, with applications to brane stabilization, domain walls, and graviton localization.

Contribution

It introduces a novel first-order approach for scalar-gravity equations in five dimensions, applicable to brane-world scenarios without requiring supersymmetry.

Findings

Successfully stabilizes inter-brane spacing with fine-tuning.

Constructs smooth domain wall solutions approaching localized branes.

Shows existence of a massless graviton mode in compactified models.

Abstract

A method for obtaining solutions to the classical equations for scalars plus gravity in five dimensions is applied to some recent suggestions for brane-world phenomenology. The method involves only first order differential equations. It is inspired by gauged supergravity but does not require supersymmetry. Our first application is a full non-linear treatment of a recently studied stabilization mechanism for inter-brane spacing. The spacing is uniquely determined after conventional fine-tuning to achieve zero four-dimensional cosmological constant. If the fine-tuning is imperfect, there are solutions in which the four-dimensional branes are de Sitter or anti-de Sitter spacetimes. Our second application is a construction of smooth domain wall solutions which in a well-defined limit approach any desired array of sharply localized positive-tension branes. As an offshoot of the analysis we suggest a construction of a supergravity c-function for non-supersymmetric four-dimensional renormalization group flows. The equations for fluctuations about an arbitrary scalar-gravity background are also studied. It is shown that all models in which the fifth dimension is effectively compactified contain a massless graviton. The graviton is the constant mode in the fifth dimension. The separated wave equation can be recast into the form of supersymmetric quantum mechanics. The graviton wave-function is then the supersymmetric ground state, and there are no tachyons.