For a transitive finite -set with at least two points, the augmentation subrepresentation of a permutation representation is irreducible if and only if the action is two-transitive. Indeed, writing the permutation character as gives
The augmentation subrepresentation is irreducible exactly when this norm is two. By the character norm of a permutation representation, that means that the diagonal and the off-diagonal are the only two orbits on , which is exactly two-transitivity.
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.
Assume . The place-permutation action on preserves the coefficient-sum kernel
It is the augmentation subrepresentation of a permutation representation. The point action of is two-transitive, so the irreducible augmentation criterion for a transitive group action makes irreducible. The two-row Young permutation module decomposition of identifies its nontrivial summand as . Hence .
All standard Young tableaux of shape are , , with below the first cell and the remaining entries increasing along the first row. Their content vectors of standard Young tableaux are
An explicit orthonormal basis realizing these tableau lines is
The sums of their coordinates vanish. Their norms are one, and the inner product of with , , is zero because the coefficients of sum to zero. Directly summing the action of gives .
For , . For , its only nontrivial two-dimensional block is
Every other is fixed, including all with when . These formulas follow by swapping coordinates in the displayed vectors, and are the Young orthogonal form with axial distance for .
The vector
is fixed by every element of , so is a trivial representation. The coefficient-sum subspace
is also -invariant, and every vector has a unique decomposition into a constant vector and an element of . Hence
Here is the augmentation subrepresentation of a permutation representation.