Recurrent tensor

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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

  1. ^ Alekseevsky, Baum (2008)
  2. ^ Weyl (1918)
  3. ^ Folland (1970)
  4. ^ Walker (1948)

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.