Permutation Tensor

The permutation tensor, also called the Levi-Civita tensor or isotropic tensor of rank 3 (Goldstein 1980, p. 172), is a pseudotensor which is antisymmetric under the interchange of any two slots. Recalling the definition of the permutation symbol in terms of a scalar triple product of the Cartesian unit vectors,

 epsilon_(ijk)=x_i^^·(x_j^^xx_k^^)=[x_i^^,x_j^^,x_k^^],
(1)

the pseudotensor is a generalization to an arbitrary basis defined by

epsilon_(alphabeta...mu)=sqrt(|g|)[alpha,beta,...,mu]
(2)
epsilon^(alphabeta...mu)=([alpha,beta,...,mu])/(sqrt(|g|)),
(3)

where

 [alpha,beta,...,mu]={1   the arguments are an even permutation; -1   the arguments are an odd permutation; 0   two or more arguments are equal,
(4)

and g=det(g_(alphabeta)), where g_(alphabeta) is the metric tensor. epsilon(x_1,...,x_n) is nonzero iff the vectors are linearly independent.

When viewed as a tensor, the permutation symbol is sometimes known as the Levi-Civita tensor. The permutation tensor epsilon^(alphabetadeltagamma) of rank four is important in general relativity, and has components defined as

 (epsilon)^(alphabetagammadelta)={+1   if alphabetagammadelta is an even permutation of 0123; -1   if alphabetagammadelta is an odd permutation of 0123; 0   otherwise
(5)

(Weinberg 1972, p. 38). The rank four permutation tensor satisfies the identity

 epsilon_(alphabetagammadelta)=-epsilon^(alphabetagammadelta).
(6)

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