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Curvature collineation

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Vector field that preserves the Riemann tensor

A curvature collineation (often abbreviated to CC) is vector field which preserves the Riemann tensor in the sense that,

L X R a b c d = 0 {\displaystyle {\mathcal {L}}_{X}R^{a}{}_{bcd}=0}

where R a b c d {\displaystyle R^{a}{}_{bcd}} are the components of the Riemann tensor. The set of all smooth curvature collineations forms a Lie algebra under the Lie bracket operation (if the smoothness condition is dropped, the set of all curvature collineations need not form a Lie algebra). The Lie algebra is denoted by C C ( M ) {\displaystyle CC(M)} and may be infinite-dimensional. Every affine vector field is a curvature collineation.

See also


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