The unique symmetric and antisymmetric decomposition is , . Both pieces are Cartesian tensors: transposing gives , so and . Hence this is a decomposition into a symmetric tensor and an antisymmetric second-rank tensor, rather than just a decomposition of numerical arrays.
For the axial vector of an antisymmetric second-rank tensor, contract the two Levi-Civita symbols:
Thus
With this convention , so the displayed matrix is the negative of the cross-product matrix for .