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TheoremStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-12
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Integrability criterion for simple highest weight kac moody modules

Statement

For every finite GCM over C and every λh, the simple highest-weight module LA(λ) is integrable if and only if λP+. Symmetrizability is not required.

Facts & Assumptions

Given: The finite GCM and weight λ.

[F1]

Every nonzero integrable highest-weight module has dominant integral highest weight (Dominance is necessary for an integrable highest weight module).

[F2]

For dominant λ, the quotient of the Verma module by N=iU(g)fiλ(hi)+1v is nonzero, highest weight and integrable (Simple root power relations generate the integrable quotient).

[F3]

The Verma module has a unique maximal proper submodule Nλ, containing every proper submodule, and LA(λ)=MA(λ)/Nλ is nonzero highest weight (Kac moody verma module has a unique simple quotient).

Proof

1.1

If LA(λ) is integrable, its nonzero highest vector is supplied by F3, so F1 gives λP+. This implication excludes no boundary label: zero labels are permitted in P+.

F1F3given
1.2

Conversely let λP+. F2 makes N proper, so NNλ by F3. Consequently the quotient map factors as a surjection MA(λ)/NLA(λ). If a simple generator has a power killing a vector upstairs, the same power kills its image. Every vector downstairs has a preimage, so both ei and fi act locally nilpotently on LA(λ).

F2F3given
2.1

The quotient also retains a weight decomposition. To see this directly, a submodule of a weight module contains every weight component of each of its elements: for finitely many distinct weights choose a Cartan element separating them and apply its Lagrange interpolation polynomials. Existence follows because finitely many nonzero linear functionals cannot vanish everywhere over the infinite field C; explicitly their evaluations on a=1dta1ha in a finite Cartan basis exclude only finitely many t. The quotient is therefore the direct sum of quotient weight spaces. Applied to the kernel in 1.2, this supplies the remaining integrability condition. With both nilpotences established there, sufficiency follows. All arguments permit N=0, zero labels and one-dimensional quotients. The simple quotient itself is never zero by F3. The empty interpolation product is 1 when only one weight occurs. No choice principle or symmetrizer is used in either direction.

F2F3step 1.2

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