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Einstein's equations in the presence of signature change

J. Math. Phys. 37, 5627 (1996); doi:10.1063/1.531730

Issue Date: November 1996

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Tevian Dray
Department of Mathematics, Oregon State University, Corvallis, Oregon 97331
Department of Physics and Mathematical Physics, University of Adelaide, Adelaide, SA 5005, Australia
School of Physics and Chemistry, Lancaster University, Lancaster LA1 4YB, United Kingdom

We discuss Einstein's field equations in the presence of signature change using variational methods, obtaining a generalization of the Lanczos equation relating the distributional term in the stress tensor to the discontinuity of the extrinsic curvature. In particular, there is no distributional term in the stress tensor, and hence no surface layer, precisely when the extrinsic curvature is continuous, in agreement with the standard result for constant signature. ©1996 American Institute of Physics.
History: Received 15 April 1996; accepted 19 June, 1996
Permalink: http://link.aip.org/link/?JMAPAQ/37/5627/1
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KEYWORDS and PACS

Keywords
PACS
  • 02.30.Wd
    Mathematical methods in physics Function theory, analysis Calculus of variations and optimal control
  • 02.10.Sp
    Mathematical methods in physics Logic, set theory, and algebra Linear and multilinear algebra; matrix theory (finite and infinite)
  • 04.20.Fy
    General relativity and gravitation Classical general relativity Canonical formalism, Lagrangians, and variational principles
  • 04.20.Jb
    General relativity and gravitation Classical general relativity Exact solutions
  • YEAR: 1996

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0022-2488 (print)   1089-7658 (online)
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REFERENCES (26)

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