2004
DOI: 10.1142/1729
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Symmetries and Curvature Structure in General Relativity

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Cited by 363 publications
(695 citation statements)
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“…Let B m denote the range space of f at m (suitably interpreted according to the agreed identification of bivectors) so that dim B m equals the curvature rank at m and is ≤ 6. This leads to a convenient algebraic classification of Riem at m into five mutually exclusive and disjoint curvature classes (for further details, see [10]). …”
Section: Curvature Structure Of Space-timesmentioning
confidence: 99%
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“…Let B m denote the range space of f at m (suitably interpreted according to the agreed identification of bivectors) so that dim B m equals the curvature rank at m and is ≤ 6. This leads to a convenient algebraic classification of Riem at m into five mutually exclusive and disjoint curvature classes (for further details, see [10]). …”
Section: Curvature Structure Of Space-timesmentioning
confidence: 99%
“…A space-time (M, g) (or some subset of it) which has the same curvature class at each point of M is said to be of that class. The subset of M consisting of points at which the curvature class is A is an open subset of M ( [10], p 393) and the analogous subset arising from the class O is closed (and has empty interior in the manifold topology of M if (M, g) is non-flat). It is important in what is to follow that the equation R abcd k d = 0 at m has no non-trivial solutions for k ∈ T m M if the curvature class at m is A or B, a unique independent solution (the vector r above) if the curvature class at m is C and two independent solutions if the curvature class at m is D (and which span the blade of * F in (3)).…”
Section: Class O In This Case Riem Vanishes At Mmentioning
confidence: 99%
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