Conjugacy classes in the symmetric group are specified by cycle type, equivalently a partition of . If counts cycles of length , the number of permutations of that cycle type is : cyclic rotation of each cycle and interchange of equal-length cycles do not change the permutation. This gives
The sizes sum to . Since the number of complex irreducible representations of a finite group equals its number of conjugacy classes, has inequivalent complex irreducible representations.
The trivial representation and sign of a permutation give
They are one-dimensional representations, hence irreducible representations. Their characters, in the conjugacy class order of solution, are
These are the only one-dimensional representations. All transpositions are conjugate, so they have the same scalar image in any one-dimensional representation; since a transposition squares to the identity, . Transpositions generate the symmetric group, fixing the whole representation once is chosen.
By the sum of squares of irreducible representation dimensions, the three remaining dimensions satisfy , with each . No can be at least , since . Thus the only possible dimensions are
Use the composition convention . Then . Since the sign of a permutation is multiplicative, the same calculation gives . Both send the identity to and have inverses given by , so both are group representations.
The trace of a permutation matrix counts fixed points, and multiplying that matrix by its sign of a permutation multiplies its trace by that sign. Thus the two characters are
Let and . Both are invariant subspaces, and . On , is the trivial representation and is the sign representation. Subtracting their characters yields
The character inner product verifies that it is an irreducible representation:
The squares of the entries of are identical, so its character inner product with itself is also one. Their values at a transposition differ, so these irreducible representations are inequivalent. Therefore
Only the character of the two-dimensional irreducible representation remains unknown. Write it as . The regular representation has character zero off the identity and decomposes with multiplicities equal to the irreducible representation dimensions. Thus, for a nonidentity element ,
For the four nonidentity conjugacy classes this gives , , , . The complete character table is consequently
For example, , agreeing with character orthogonality.
Use the realization from solution. Put , which identifies the three-dimensional scalar field with . The polynomial invariants of the standard S4 representation include the symmetric power sums
because every permutation merely rearranges their summands. In these coordinates,
Neither polynomial vanishes identically: at they equal and . Hence coefficients multiplying and provide nonzero invariant quadratic and cubic terms. A change of basis transports these polynomial invariants to any equivalent realization of . For a real scalar field, both are real. For a complex scalar field, a real scalar potential may contain ; the quadratic Hermitian form is another invariant.
As an independent character check, the symmetric square of a group representation has character , and the symmetric cube of a group representation has character . With these are and . Their character inner products with are both one, so each degree has exactly one independent polynomial invariant.

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