Scalar field cosmology in three-dimensions
We study an analytical solution to the Einstein's equations in 2 + 1-dimensions. The space-time is dynamical and has a line symmetry. The matter content is a minimally coupled, massless, scalar field. Depending on the value of certain parameters, this solution represents three distinct space-times. The first one is at space-time. Then, we have a big bang model with a negative curvature scalar and a real scalar field. The last case is a big bang model with event horizons where the curvature scalar vanishes and the scalar field changes from real to purely imaginary.
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Sociedade Brasileira de Física
2001
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oai:scielo:S0103-973320010003000172015-11-26Scalar field cosmology in three-dimensionsOliveira-Neto,G.We study an analytical solution to the Einstein's equations in 2 + 1-dimensions. The space-time is dynamical and has a line symmetry. The matter content is a minimally coupled, massless, scalar field. Depending on the value of certain parameters, this solution represents three distinct space-times. The first one is at space-time. Then, we have a big bang model with a negative curvature scalar and a real scalar field. The last case is a big bang model with event horizons where the curvature scalar vanishes and the scalar field changes from real to purely imaginary.info:eu-repo/semantics/openAccessSociedade Brasileira de FísicaBrazilian Journal of Physics v.31 n.3 20012001-09-01info:eu-repo/semantics/articletext/htmlhttp://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-97332001000300017en10.1590/S0103-97332001000300017 |
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Oliveira-Neto,G. Scalar field cosmology in three-dimensions |
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Oliveira-Neto,G. |
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Oliveira-Neto,G. |
title |
Scalar field cosmology in three-dimensions |
title_short |
Scalar field cosmology in three-dimensions |
title_full |
Scalar field cosmology in three-dimensions |
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Scalar field cosmology in three-dimensions |
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Scalar field cosmology in three-dimensions |
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scalar field cosmology in three-dimensions |
description |
We study an analytical solution to the Einstein's equations in 2 + 1-dimensions. The space-time is dynamical and has a line symmetry. The matter content is a minimally coupled, massless, scalar field. Depending on the value of certain parameters, this solution represents three distinct space-times. The first one is at space-time. Then, we have a big bang model with a negative curvature scalar and a real scalar field. The last case is a big bang model with event horizons where the curvature scalar vanishes and the scalar field changes from real to purely imaginary. |
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Sociedade Brasileira de Física |
publishDate |
2001 |
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http://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-97332001000300017 |
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AT oliveiranetog scalarfieldcosmologyinthreedimensions |
_version_ |
1756407240642789376 |