For a finite group , subgroups , and a complex group representation of , the Mackey restriction formula isChoose one representative of each double coset . The conjugate subgroup representation is a representation of on the same vector space, with . Restriction of a representation keeps the vector space and restricts the acting subgroup. induced representation is , and analogously for each subgroup of . The displayed isomorphism is an isomorphism of -representations. These definitions specify every summand and its subgroup.
If is -transitive, it is transitive by extending one-element tuples to -tuples. Apply -transitivity to tuples beginning with to see that the stabilizer subgroup is -transitive on the remaining elements.
Conversely, given two ordered -tuples of distinct elements, transitivity first supplies carrying their first entries to each other. Conjugating the given stabilizer hypothesis shows that the stabilizer of the target first entry is -transitive. An element of that stabilizer then maps the remaining entries of the image tuple to their targets. Composing the two elements proves -transitivity. For , the condition on zero-tuples is vacuous.
For finite nonempty , let be the basis vectors of the permutation representation. PutThe line is fixed by , and is the augmentation subrepresentation of a permutation representation. Since in , they have zero intersection and their dimensions add to . Hence .
The printed formulation does not explicitly require to be finite. For an infinite nonempty -set, interpret as finite-support vectors. Choose one finite orbit (all orbits are finite because is finite), replace by , and use the same augmentation kernel. This again splits off a trivial summand. The nonempty-set assumption is needed; the empty permutation module contains no trivial summand.
As printed, the equivalence needs a transitivity hypothesis. A group acting trivially on two points has , so is one-dimensional and irreducible, although the action is not even transitive.
Here is the intended result for a transitive action. The set is then finite, and, for a point stabilizer , its permutation character is . Frobenius reciprocity givesThe last equality follows because an -fixed vector has constant coefficients on each orbit. There is exactly one trivial constituent, since the action is transitive. Therefore, writing for the character of ,By character orthogonality, is irreducible exactly when this equals . One stabilizer orbit is , so this happens exactly when is transitive on , equivalently when is two-transitive. Moreover is not trivial, since a transitive action has only one independent fixed vector in the whole permutation module.
The complete correction without assuming transitivity is also precise: is irreducible exactly for a two-transitive action or the exceptional action on two fixed points. Indeed for a finite set with orbits, the fixed subspace of has dimension . If and is irreducible, must itself be a one-dimensional trivial module, forcing and . If is infinite, is infinite-dimensional and cannot be irreducible: any nonzero vector generates a submodule of dimension at most .
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