The Weyl tensor is the tensor defined by
|
(1)
|
where is the Riemann
tensor,
is the scalar curvature, is the metric tensor,
and denotes the antisymmetric
tensor part (Wald 1984, p. 40).
The Weyl tensor is defined so that every tensor
contraction between indices gives 0. In particular,
|
(2)
|
(Weinberg 1972, p. 146). The number of independent components for a Weyl tensor in -D for is given by
|
(3)
|
(Weinberg 1972, p. 146). For , 4, ..., this gives 0, 10, 35, 84, 168, ... (OEIS A052472).
See also
Scalar Curvature,
Riemann
Tensor
Explore with Wolfram|Alpha
References
Eisenhart, L. P. Riemannian Geometry. Princeton, NJ: Princeton University Press, 1964.Parker,
L. and Christensen, S. M. "The Ricci, Einstein, and Weyl Tensors."
§2.7.1 in MathTensor:
A System for Doing Tensor Analysis by Computer. Reading, MA: Addison-Wesley,
pp. 30-32, 1994.Sloane, N. J. A. Sequence A052472
in "The On-Line Encyclopedia of Integer Sequences."Wald, R. M.
General
Relativity. Chicago, IL: University of Chicago Press, 1984.Weinberg,
S. Gravitation
and Cosmology: Principles and Applications of the General Theory of Relativity.
New York: Wiley, 1972.Weyl, H. "Reine Infinitesimalgeometrie."
Math. Z. 2, 384-411, 1918.Referenced on Wolfram|Alpha
Weyl Tensor
Cite this as:
Weisstein, Eric W. "Weyl Tensor." From
MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/WeylTensor.html
Subject classifications