The symmetric power is the quotient of identifying tensors which differ by permutation of the factors. The exterior power is the alternating quotient, with a tensor having repeated equal factors set to zero. Both quotients inherit the given group action. For a basis , bases consist respectively of monomials with , and wedge products with . Thus
with the second dimension zero for .
A finite-order group element is diagonalizable over , because its minimal polynomial divides , which has no repeated roots. Choose an eigenbasis with eigenvalues . The induced eigenvalues, including multiplicities, are
The zeroth powers are the one-dimensional trivial representation, with the empty product equal to .

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