# Riemann tensor

Riemann curvature tensor

A four-valent tensor that is studied in the theory of curvature of spaces. Let be a space with an affine connection and let be the Christoffel symbols (cf. Christoffel symbol) of the connection of . The components (coordinates) of the Riemann tensor, which is once contravariant and three times covariant, take the form  where is the symbol of differentiation with respect to the space coordinate , . In a Riemannian space with a metric tensor , in addition to the tensor the four times covariant Riemann tensor obtained by lowering the upper index using the metric tensor is also studied   Here since the Riemannian connection (without torsion) is considered on . In an arbitrary space with an affine connection without torsion the coordinates of the Riemann tensor satisfy the first Bianchi identity  i.e. the cyclic sum with respect to the first three subscripts is zero.

The Riemann tensor possesses the following properties:

1) ;

2) ;

3) , ;

4) , , if both subscripts of one pair are identical, then the corresponding coordinate equals zero: ;

5) the second Bianchi identity is applicable to the absolute derivatives of the Riemann tensor: where is the symbol for covariant differentiation in the direction of the coordinate . The same identity is applicable to the tensor .

A Riemann tensor has, in all, coordinates, being the dimension of the space, among which are essential. Between the latter no additional dependencies result from the properties listed above.

When the Riemann tensor has one essential coordinate, ; it forms part of the definition of the intrinsic, or Riemannian, curvature of the surface: (see Gaussian curvature).

The Riemann tensor was defined by B. Riemann in 1861 (published in 1876).

How to Cite This Entry:
Riemann tensor. L.A. Sidorov (originator), Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Riemann_tensor&oldid=15143
This text originally appeared in Encyclopedia of Mathematics - ISBN 1402006098