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The Murnaghan expansion at every admissible rank

Statement

For all partitions α,β and every integer n≥max⁡{∣α∣+α1, ∣β∣+β1}: sα[n]∗sβ[n]=∑γgˉα,βγ sγ[n], an identity in the symmetric function ring, where sγ[n] is the Jacobi–Trudi determinant attached to the integer sequence γ[n]=(n−∣γ∣,γ1,γ2,… ), equal to 0 or ±1 times a Schur function (The Jacobi–Trudi completion sμ, the operators Un and V, and stab⁡(α,β), First-row padding of a partition), and ∗ is the internal product (Kronecker coefficients and the internal tensor product).

For an ordinary partition δ⊢n the coefficient of sδ is gα[n],β[n]δ=∑γgˉα,βγ ⟨sγ[n],sδ⟩H, where each Hall factor is 0 or a sign coming from Jacobi–Trudi straightening (Schur functions form an orthonormal integral basis). At small admissible ranks the signed terms can cancel or coalesce; individual coefficients need not yet equal their reduced values. The range displayed is precisely the set of n for which α[n] and β[n] are partitions.

Facts & Assumptions

Given: Partitions α,β,γ,δ with δ⊢n, and integers k≥0.

[F1]

Rα,β=∑γgˉα,βγsγ, a finite Schur expansion (Brion's formula for the reduced Kronecker coefficients, The reduced (stable) Kronecker coefficient gˉα,βγ).

[F2]

(Unsα)∗(Unsβ)=UnRα,β for every n≥0, including nonadmissible ranks, and ∑n≥0(Unsα)∗(Unsβ)tn=σ[tX]Rα,β[tX−1] (The Jacobi–Trudi completion is compatible with the internal product).

[F3]

Un(sλ)=sλ[n] on the Schur basis and Un is Z-linear; for n≥∣α∣+α1 the sequence α[n] is a partition and Unsα=sα[n] is the honest Schur function (The Jacobi–Trudi completion sμ, the operators Un and V, and stab⁡(α,β), First-row padding of a partition).

[F4]

sμ∗sν=∑δgμ,νδsδ for partitions of equal size, the Schur basis is orthonormal, and sγ[n] is an integer combination of Schur functions of degree n that is 0 or ±1 times a Schur function (Kronecker coefficients and the internal tensor product, Schur functions form an orthonormal integral basis, The Jacobi–Trudi completion sμ, the operators Un and V, and stab⁡(α,β)).

[F5]

The vertex-operator series identifies the coefficients of σ[tX]Rα,β[tX−1], so UnRα,β is the coefficient of tn there (Vertex-operator generating series for the padded Schur functions).

[F6]

The finite Littlewood expression for Rα,β is given in The Jacobi–Trudi completion is compatible with the internal product; LR coefficients count lattice semistandard tableaux (The Littlewood–Richardson rule for products of Schur functions, Littlewood--Richardson tableaux and coefficients), and s(m) is the internal-product unit in degree m (The internal (Kronecker) product on symmetric functions).

Proof

technique · direct
1.1F1

By [F1], Rα,β=∑γgˉα,βγsγ with finitely many nonzero terms.

1.2F1F6

Local reduced coefficients for (2),(2). In the Littlewood expression of [F6], (sδsτ)⊥s(2) is nonzero only when δ=(m) and τ=(r) are rows with m+r≤2 (a row LR target forces every factor to be a row); it then equals s(2−m−r). The analogous condition holds for ϵ, and sδ∗sϵ=0 unless their degrees agree, in which case it is s(m) by the unit rule. Here (0) means ∅. Hence R(2),(2)=∑m+r≤2s(2−m−r)2s(m)=s(2)2+s(1)2+1+s(1)3+s(1)+s(2). Counting row LR tableaux gives s(2)2=s(4)+s(3,1)+s(2,2) and s(1)2=s(2)+s(1,1); adding one box to these two shapes gives s(1)3=s(3)+2s(2,1)+s(1,1,1). Thus R(2),(2)=1+s(1)+2s(2)+s(1,1)+s(1,1,1)+2s(2,1)+s(2,2)+s(3)+s(3,1)+s(4), whose coefficients are exactly the reduced coefficients by [F1].

2.1F2F3F5step 1.1

By [F2], (Unsα)∗(Unsβ)=UnRα,β for every n≥0; by [F5], UnRα,β is the coefficient of tn in σ[tX]Rα,β[tX−1], and since Un is Z-linear with Un(sγ)=sγ[n] by [F3], it equals ∑γgˉα,βγsγ[n], a finite sum. Hence the displayed identity holds for every n≥0 at the level of Jacobi–Trudi completions.

3.1F3step 2.1

In the admissible range n≥max⁡{∣α∣+α1,∣β∣+β1} the padded sequences α[n],β[n] are partitions, so by [F3] the left side of step 2.1 is the internal product sα[n]∗sβ[n] of two honest Schur functions; this proves the first display in exactly the stated range and shows that the range is the full set of n for which both inputs are partitions.

3.2F3F4step 2.1step 1.2

Rank-four cancellation. Apply U4 to the ten terms of step 1.2. The tails ∅,(1),(2),(1,1),(1,1,1) give s(4),s(3,1),s(2,2),s(2,1,1),s(1,1,1,1) respectively. The tails (2,1),(2,2) give zero by repeated straightening indices. The tails (3),(3,1),(4) give −s(2,2),−s(2,1,1),−s(3,1) respectively by [F3]–[F4]. With their multiplicities from step 1.2, the sum is s(4)+s(1,1,1,1)+s(2,2); in particular its (2,2) coefficient is 2−1=1, whereas the reduced (2) coefficient is 2. This proves the announced cancellation locally.

4.1F4step 3.1

Coefficient form. For δ⊢n, pair the identity of step 2.1 against sδ using orthonormality [F4]: the left side gives ⟨sα[n]∗sβ[n],sδ⟩H=gα[n],β[n]δ by [F4], and the right side gives ∑γgˉα,βγ⟨sγ[n],sδ⟩H, where each factor is a Hall pairing of the Jacobi–Trudi determinant sγ[n] with a Schur function, hence a signed multiplicity of a Schur constituent, 0 or ±1 by [F4]. This is the second display, and it shows that individual coefficients can receive both positive and negative contributions from different γ and need not equal gˉα,βγ.

5.1F1F2step 4.1∎

Choice and finiteness. Every step uses finite sums: the Schur expansion of Rα,β is finite by [F1], the sum over γ in step 2.1 is finite, and the coefficient extraction of step 4.1 uses the finite degree-n part of the Schur basis. No form of the axiom of choice is used; the identity is asserted for all admissible ranks, not only for the eventually stable ones.

Remark

For α=β=(2), every rank n≥4 product is UnR(2),(2), where R(2),(2)=1+s(1)+2s(2)+s(1,1)+s(1,1,1)+2s(2,1)+s(2,2)+s(3)+s(3,1)+s(4). Its coefficients are the reduced coefficients, and all other reduced coefficients vanish. This finite polynomial and its rank-four cancellation are proved in steps 1.2 and 3.2 above.

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