2007
DOI: 10.1007/s10714-007-0411-9
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Exact solutions for the massless plane symmetric scalar field in general relativity, with cosmological constant

Abstract: The Klein-Gordon equations are solved for the case of a planesymmetric static massless scalar field in general relativity with cosmological constant, generalizing the solutions found by Taub, Novotny and Horsky, and Singh. A separate class of solutions is obtained in which the metrics reduce to flat space in the limit that → 0. The static solutions can be used to generate time-dependent cosmological solutions, one of which exhibits rapid inflation followed by continued exponential expansion at all later times.

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Cited by 11 publications
(16 citation statements)
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References 11 publications
(12 reference statements)
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“…In four dimensions we can mention the existence of a particular plane-symmetric solution with nonzero cosmological constant (of arbitrary sign) given in [28]. Finally, a particular solution to the problem in d dimensions with a flat base manifold was found in [15].…”
mentioning
confidence: 90%
“…In four dimensions we can mention the existence of a particular plane-symmetric solution with nonzero cosmological constant (of arbitrary sign) given in [28]. Finally, a particular solution to the problem in d dimensions with a flat base manifold was found in [15].…”
mentioning
confidence: 90%
“…Now we investigate the stability of the field equations (3,4) under small pertubations.First we note that instead of working with the system (3,4) we can treat the (6,8) as the field equations.in linear approximation (6) becomes…”
Section: About the Stability Of The Field Equationsmentioning
confidence: 99%
“…Finally, a generalization of the Singh's solution with the presence of a massless plane symmetric scalar field and a cosmological constant was recently found by Vuille. [9] One particular solution which leads to the above potential in the Newtonian limit is the Rohrlich [10] solution that actually describes flat spacetime in a special coordinate system. On the other hand, in this article, we will consider the metric first found by Horský [11] which represents a truly curved spacetime.…”
Section: Introductionmentioning
confidence: 99%