Any square matrix can be written as a sum
| (1) |
where
| (2) |
is a symmetric matrix known as the symmetric part of and
| (3) |
is an antisymmetric matrix known as the antisymmetric part of . Here,
is the transpose.
The symmetric part of a tensor is denoted using parentheses as
| (4) |
| (5) |
Symbols for the symmetric and antisymmetric parts of tensors can be combined, for example
| (6) |
(Wald 1984, p. 26).