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TauCeti.RepresentationTheory.Symmetric.TensorAction.Faithful

How faithfully the symmetric group acts on a tensor power #

The symmetric group S_d acts on (Rⁿ)^{⊗d} by permuting tensor factors, and that action extends to an algebra map R[S_d] → End((Rⁿ)^{⊗d}). Over a nontrivial commutative ring, this file measures how much of R[S_d] survives: the algebra map is injective exactly when d ≤ n.

Above the threshold the tensor power is too small to separate permutations linearly. For n < d every monomial basis vector of (Rⁿ)^{⊗d} repeats one of its factors, so the full antisymmetrizer ∑_σ sgn(σ) σ acts as 0 over every commutative ring, and is nonzero when the ring is nontrivial. This is why Schur--Weyl duality is stated for the image of R[S_d] in End((Rⁿ)^{⊗d}) rather than for R[S_d] itself.

Over a nontrivial commutative semiring, the group-level question has a different, coarser answer, recorded here as well: the permutation representation itself is faithful as soon as Rⁿ has two independent coordinate directions with which to tell tensor slots apart, that is, exactly when 2 ≤ n or d ≤ 1.

Both answers are read off the monomial basis tensorPowerBasis of (Rⁿ)^{⊗d}, indexed by the functions Fin d → Fin n, on which a permutation acts by precomposition with its inverse.

Main results #

References #

Faithfulness of the symmetric-group image. If the tensor degree does not exceed the dimension, the algebra map R[S_d] → End((Rⁿ)^{⊗d}) is injective.

The antisymmetrizer dies below the threshold. If the dimension is smaller than the tensor degree, then every monomial basis vector of (Rⁿ)^{⊗d} repeats a factor, and the full antisymmetrizer ∑_σ sgn(σ) σ annihilates the whole tensor power.

Non-faithfulness above the threshold. If the dimension is smaller than the tensor degree, the algebra map R[S_d] → End((Rⁿ)^{⊗d}) has a nonzero kernel, so the symmetric-group image is a proper quotient of the group algebra.

The faithfulness threshold. The algebra map R[S_d] → End((Rⁿ)^{⊗d}) is injective exactly when the tensor degree does not exceed the dimension.

theorem TauCeti.permTensorAction_eq_one_of_le_one {R : Type u} {n d : ℕ} [CommSemiring R] (h : n ≤ 1) (σ : Equiv.Perm (Fin d)) :
(permTensorAction R n d) σ = 1

With at most one coordinate direction the tensor slots cannot be told apart, and the permutation action on (Rⁿ)^{⊗d} is trivial.

With at least two coordinate directions the permutation action on (Rⁿ)^{⊗d} is faithful: the monomial basis vector marking a single tensor slot already detects the permutation.

When the permutation representation itself is faithful. Unlike the group-algebra image, the representation of S_d on (Rⁿ)^{⊗d} is faithful for every tensor degree once 2 ≤ n; it fails only when the dimension collapses the action while there is more than one slot to permute.