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Harish-Chandra isomorphism for the center

Statement

Assume the Axiom of Choice. Let g be a finite-dimensional complex semisimple Lie algebra, let h be any Cartan subalgebra in the nilpotent self-normalizing sense, and fix a positive root system with Weyl group W and half-sum ρ of its positive roots. The shifted Harish-Chandra map

HC⁡ρ ⁣:Z(U(g))→S(h)W,HC⁡ρ(z)(λ)=pr⁡(z)(λ−ρ),

is an algebra isomorphism.

Facts & Assumptions

Given: The Axiom of Choice, a finite-dimensional complex semisimple Lie algebra g, any Cartan subalgebra h in the nilpotent self-normalizing sense, a positive root system and its W,ρ, and the shifted Harish-Chandra map HC⁡ρ(z)(λ):=pr⁡(z)(λ−ρ) on the center of U(g).

[A1]

The Axiom of Choice is The Axiom of Choice; it is inherited by the Chevalley restriction step in [F2].

[F1]

The Harish-Chandra projection is multiplicative on the center (The Harish-Chandra projection is multiplicative on the center).

[F2]

The leading PBW symbol of a central element is invariant, and under [A1] Chevalley restriction identifies symmetric invariants on g with Weyl invariants on this arbitrary Cartan h (The leading PBW symbol of a central element is invariant, Chevalley restriction for symmetric invariants).

Proof

technique · direct
1.1F1given

Let fz(μ):=pr⁡(z)(μ) for z∈Z(U(g)). Multiplicativity from [F1] shows that HC⁡ρ(z)(λ)=fz(λ−ρ) defines an algebra homomorphism. To identify its image, fix a simple reflection si and a weight μ with ⟨μ+ρ,αi∨⟩=m∈Z>0. Work in the Verma module M(μ). By The simple-root singular vector in a Verma module, fimvμ is a nonzero highest-weight vector of weight si⋅μ. The central element z acts on all of M(μ) by the scalar fz(μ), while The Harish-Chandra projection computes the highest-weight scalar applied to the cyclic submodule generated by this singular vector gives the scalar fz(si⋅μ). Thus they are equal. The weights with m∈Z>0 are Zariski dense: a polynomial vanishing on all these infinitely many parallel hyperplanes vanishes identically. Hence fz is invariant under the dot action of every simple reflection, and therefore under W. By The rho-shift intertwines the dot and ordinary Weyl actions, HC⁡ρ(z) lies in S(h)W.

2.1step 1.1

The PBW filtration on U(g) induces a filtration on the center, and the Harish-Chandra projection does not increase PBW degree because it is defined by projecting the PBW decomposition onto the U(h) summand. Translation by ρ preserves polynomial degree on S(h), so HC⁡ρ is a filtered algebra homomorphism.

3.1step 2.1algebra

The PBW theorem gives the symmetrization map sym⁡:S(g)→U(g),x1⋯xm↦1m!∑σ∈Smxσ(1)⋯xσ(m), as a filtration-preserving vector-space isomorphism whose associated graded map is the identity. The adjoint action is a derivation on both sides, so sym⁡ is g-equivariant. Since an element of U(g) is central exactly when it is killed by the adjoint action of the generators g, symmetrization restricts to invariant lifts and gives gr⁡Z(U(g))=S(g)g. PBW gives an ordered monomial basis for the enveloping algebra

4.1A1F2step 3.1algebra

In the PBW decomposition, the top-degree part of pr⁡(z) is obtained by discarding every monomial whose symbol contains a factor from n− or n+. Translation by ρ changes only lower-degree terms. Thus the associated-graded Harish-Chandra map is exactly restriction S(g)g⟶S(h)W, which is an isomorphism by [A1, F2].

5.1step 2.1step 4.1∎

A filtered algebra homomorphism whose associated graded map is an isomorphism is itself an isomorphism: lift target elements degree by degree for surjectivity, and take the leading symbol of a kernel element for injectivity. Applying this to steps 2.1 and 4.1 shows that HC⁡ρ is an algebra isomorphism Z(U(g))→∼S(h)W.

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