For a finite group , subgroups , and a complex group representation of , the Mackey restriction formula is
Choose 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. Put
The 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 gives
The 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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