Tensor derivative

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1 Definition

Let M be a smooth manifold and E,E' vector bundles over M, both equipped with a covariant derivative \nabla. Then the vector bundle \textup{Hom}(E,E') of bundle homomorphisms (sometimes called tensors) inherits another covariant derivative \nabla : \Gamma TM \times \Gamma\textup{Hom}(E,E') \to \Gamma\textup{Hom}(E,E') called the tensor derivative which is defined as follows:

(1)(\nabla_XT)s = \nabla_X(Ts) - T(\nabla_Xs)

for any X \in \Gamma TM and s\in \Gamma E. The definition is made such that the application of tensors (sections in \textup{Hom}(E,E')) to sections in E satisfies the Leibniz product rule:

(2)\nabla_X(Ts) = (\nabla_XT)s + T(\nabla_Xs)

The corresponding curvature tensors of the bundles E, E' and \textup{Hom}(E,E') are related similarly:

(3)(R(X,Y)T)s = R(X,Y)Ts - T(R(X,Y)s)

for any X,Y \in \Gamma TM and s\in \Gamma E.

A tensor T \in \Gamma\Hom(E,E') is called parallel if its tensor derivative vanishes, \nabla_X T = 0 for all X \in \Gamma TM.

2 Examples

  • A (semi-)Riemannian metric g \in \Gamma\Hom(S^2TM,\R) is parallel for its Levi-Civita connection.
  • A Riemannian manifold has parallel curvature tensor R \in \Gamma\Hom(\Lambda^2TM,\textup{End}(TM)) iff it is locally symmetric.
  • A submanifold M \subset \R^n has parallel second fundamental form \alpha \in \textup{Hom}(S^2TM,NM) iff M is locally extrinsic symmetric.

For further information see [Husemoller1994] and [Kobayashi&Nomizu1963].

3 References

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