This article has multiple issues. Please help improve it or discuss these issues on the talk page. (Learn how and when to remove these messages)
No issues specified. Please specify issues, or remove this template. |
In mathematics, a recurrent tensor with respect to a connection on a manifold M is a tensor T for which there is a one-form ω on M such that
Examples
Parallel Tensors
An Example for recurrent tensors are parallel tensors which are defined by
with respect to some connection .
If we take a pseudo-Riemannian manifold then the metric g is a parallel and therefore recurrent tensor with respect to its Levi-Civita connection, which is defined via
and its property to be torsion-free.
Important tensors are recurrent vector fields such as parallel vector fields ( ) which are important in mathematic research. A result for recurrent vector fields on a pseudo-Riemannian manifold is the following. Let be a recurrent vectorfield satisfying
for some one-form . Now if ( closed), e.g. if the length of is not vanishing, X can be rescaled to a parallel vectorfields [1]. In particular non parallel, recurrent vector fields are lightlike vektorfields.
Metric space
Another example for a recurrent tensor appears in connection with Weyl structures. Historical Weyl structures emerge from consideration of Hermann Weyl on properties of parallel transport of vectors and their length [2]. By claiming a manifold to have a affine parallel transport in such a way that the manifold locally looks like an affine space he got a special property for the induced connection to have a vanashing torsion tensor
- .
In addition he claimed the manifold to have a special parallel transport of the metric or scale in every point, which does not leave length of single vectors untouched but fixes ratio of two parallel transported vectors. A connection , which induces such a parallel transport than fulfills
for some one-form . In particular is such a metric is a reccurent tensor with respect to . As a result Weyl called a manifold with affine connection and recurrent metric g a metric space. Nowadays the term metric space is used slightly more general. Accurately Weyl was not just referring to one metric but to the conformal structure defined by g which can be motivated as follows:
Under conformal changes the form changes as . This induces a canonical map on as follows:
- ,
where is the conformal structure. is called a Weyl structure [3], which more generaly is defined as a map with property
- .
Recurrent spacetime
One more example of a recurrent tensor is the curvature tensor on a recurrent spacetime [4], for which
- .
References
Literature
- Weyl, H. (1918). "Gravitation und Elektrizität". Sitzungsberichte der preuss. Akad. d. Wiss.: 465.
- A.G. Walker: On parallel fields of partially null vector spaces, The Quarterly Journal of Mathematics 1949, Oxford Univ. Press
- E.M. Patterson: On symmetric recurrent tensors of the second order, The Quarterly Journal of Mathematics 1950, Oxford Univ. Press
- J.-C. Wong: Recurrent Tensors on a Linearly Connected Differentiable Manifold, Transactions of the American Mathematical Society 1961,
- G.B. Folland: Weyl Manifolds, J. Differential Geometry 1970
- D.V. Alekseevky, H. Baum (2008). Recent developments in pseudo-Riemannian geometry. European Mathematical Society. ISBN 3-037-19051-5.