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Freudenthal recursion terminates from the highest weight

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let λ∈Λ+.

(i) mλ(λ)=1, and mλ(ν)=0 whenever ν≰λ, that is, whenever λ−ν is not a nonnegative integral combination of the simple roots (The highest-weight space is one-dimensional, Highest weight modules lie below the top weight).

(ii) If μ is a weight of L(λ) with μ≠λ, then (μ+ρ,μ+ρ)<(λ+ρ,λ+ρ) (The shifted norm of a weight is maximal only at the top weight), so Freudenthal's weight multiplicity recursion solves for mλ(μ) from the multiplicities mλ(μ+jα), j≥1, of strictly higher weights; since ht⁡(λ−(μ+jα))<ht⁡(λ−μ) and L(λ) is finite-dimensional, iterating the recursion from the top weight and increasing ht⁡(λ−μ) determines mλ(μ) for every weight μ≠λ from the value mλ(λ)=1 of (i). More explicitly, for candidates ν∈λ−Q+ put D(ν)=(λ+ρ,λ+ρ)−(ν+ρ,ν+ρ). For ν≠λ with D(ν)≤0 set mλ(ν)=0, as (ii)'s strict inequality excludes such a weight. For D(ν)>0 use the recursion, including candidates that turn out to have multiplicity zero. A requested candidate at height h requires only the finitely many candidates of height at most h.

(iii) At μ=λ the recursion reads 0=0 and determines nothing, so (i) is used as its base case; if ν≰λ then ν+jα≰λ for every α∈Φ+ and j≥1, and both sides of the recursion vanish by (i).

Facts & Assumptions

Given: The Axiom of Choice, a dominant integral weight λ∈Λ+, the finite-dimensional simple module L(λ), its multiplicities mλ(ν), the positive system Φ+ with heights, and the Weyl vector ρ.

[A1]

The Axiom of Choice is assumed; it is inherited from the published highest-weight and multiplicity suppliers of [F1] and [F2] (The Axiom of Choice).

[F1]

L(λ) is a finite-dimensional irreducible highest weight module of highest weight λ, its λ-weight space is one-dimensional, and every weight ν of L(λ) satisfies ν≤λ, that is, λ−ν∈Q+; consequently mλ(ν)=0 for ν≰λ (Highest-weight classification, The highest-weight space is one-dimensional, Highest weight modules lie below the top weight).

[F2]

For every weight μ≠λ of L(λ) the recursion coefficient (λ+ρ,λ+ρ)−(μ+ρ,μ+ρ) is strictly positive (The shifted norm of a weight is maximal only at the top weight), and the recursion of Freudenthal's weight multiplicity recursion reads ((λ+ρ,λ+ρ)−(μ+ρ,μ+ρ))mλ(μ)=2∑α∈Φ+∑j≥1(μ+jα,α)mλ(μ+jα).

[F3]

Extend root height to Q by ht⁡(∑iniαi)=∑ini. It is additive and positive on Q+∖{0}, so ht⁡(λ−(μ+jα))=ht⁡(λ−μ)−jht⁡(α)<ht⁡(λ−μ) for j≥1 and α∈Φ+, while adding jα to ν can only increase it in the root order: if ν+jα≤λ then λ−ν=(λ−ν−jα)+jα∈Q+ (Height and highest root, Finite Weyl root system, lattice and chamber conventions, Simple roots form a signed integral basis).

Proof

technique · direct
1.1F1algebraA1

By [F1] the λ-weight space of L(λ) is one-dimensional and every weight of L(λ) lies below λ, so mλ(λ)=1 and mλ(ν)=0 for every ν≰λ, which is (i).

2.1F1F2F3step 1.1algebra

For every candidate ν∈λ−Q+ put h=ht⁡(λ−ν). We determine its actual multiplicity by induction on h. At height zero the only candidate is λ, whose multiplicity is 1. At positive height, if D(ν)≤0, [F2] excludes ν from the weight set, so its multiplicity is zero. If D(ν)>0, the recursion, valid for every ν, determines its multiplicity by division by D(ν). Each term mλ(ν+jα) either vanishes because ν+jα≰λ by [F1], or is a candidate of smaller nonnegative height by [F3] and hence already determined. In the latter case jht⁡(α)≤h, so only finitely many terms are required. There are finitely many tuples of nonnegative simple-root coefficients of sum at most h; thus computing any requested candidate uses finitely many induction stages and candidates. Every actual weight is among these candidates, proving (ii).

3.1F1F2F3step 1.1step 2.1algebra∎

For (iii), at μ=λ the coefficient in [F2] vanishes because μ=λ, while λ+jα≰λ for j≥1 and α∈Φ+ since −jα∉Q+, so every multiplicity on the right vanishes by (i) and the recursion reads 0=0; for ν≰λ and j≥1 one has ν+jα≰λ by [F3], so both sides of the recursion vanish by (i).

Depends on

Used by

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