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Kostant cohomology for sl2

Example

Assume the Axiom of Choice, inherited from Kostant's theorem (The Axiom of Choice). Let g=sl2(C), with Cartan subalgebra h=CH, positive root α, Weyl vector ρ=α/2, fundamental weight ω=α/2, and λ=mω with m∈Z≥0, so that V=L(mω) has dimension m+1 and n+=Ceα. The Weyl group is {1,s} with s⋅λ=s(λ+ρ)−ρ=−λ−2ρ=−(m+2)ω. Kostant's theorem gives H0(n+,V)=Cmω,H1(n+,V)=C−(m+2)ω,Hk(n+,V)=0 (k≥2), with generators vmω and εα⊗vsλ, where vsλ∈Vsλ has weight sλ=−mω. This verifies the sign of the dot action, the ρ-shift and the top degree in the smallest rank, and shows that the degree-one weight is −(m+2)ω, not −mω.

Verification

Given: The Axiom of Choice; g=sl2(C) with the usual basis H,e,f and positive root α, the Weyl group {1,s}, a nonnegative integer m, the module V=L(mω) of dimension m+1, and n+=Ceα.

[L1] sρ=−ρ, sα=−α, and the dot action is s⋅λ=s(λ+ρ)−ρ (Root reflections and the Weyl group action, The Weyl vector rho for a chosen positive system, The special linear Lie algebra sl_2, The root sl_2 triple).

[L2] Hk(n+,V)=⨁ℓ(w)=kCw⋅λ for k=0,1 and Hk=0 for k≥2, since ∣Φ+∣=1 and the Weyl group has the two elements 1,s of lengths 0,1 (Kostant's nilradical cohomology theorem, Kostant cohomology in degrees zero and top, Length and longest Weyl-group element).

[L3] V=L(mω) is finite dimensional of dimension m+1, the weight sλ=−mω occurs in V with multiplicity one, and in degree one the extremal cochain of The extremal weight cochain of a Weyl element is closed and unique is γs=εα⊗vsλ (Finite-dimensional representations of sl_2, Weight and weight space).

1.1L1L2

1⋅λ=1(λ+ρ)−ρ=λ=mω, and by [L1] s⋅λ=s(λ+ρ)−ρ=−λ−2ρ=−mω−α=−(m+2)ω; since ∣Φ+∣=1 and ℓ(1)=0, ℓ(s)=1, [L2] gives the displayed cohomology.

1.2L1L2L3

In degree one, the generator is εα⊗vsλ: its exterior factor has weight −α and vsλ has weight sλ=−mω, so the total weight −α−mω=−(m+2)ω is the dot weight, confirming the ρ-shift; the degree-zero generator is the highest vector vmω.

2.1L2step 1.2∎

Counting: dim⁡H0=1, dim⁡H1=1, and Hk=0 for k≥2, matching the top degree ∣Φ+∣=1; the degree-one weight is −(m+2)ω=−mω−α, strictly below −mω, so the exterior root shift cannot be dropped.

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