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The cyclotomic module G0 is the restricted dual integral highest-weight module

Statement

For the same standard homogeneous general-field/general-Cartan parameters as the integral projective theorem, the tensor pairing T(P,M)=gdim⁡(Pψ⊗M) is weightwise perfect and A-bilinear, with normalized cover/simple dual bases. Its associated map Ψcan:G0(RΛ)⟶VA(Λ)∨=⨁βHom⁡A(VA(Λ)Λ−β,A),Ψcan(M)(ϕ(P))=T(P,M) is an isomorphism to the RESTRICTED weight dual, identified inside V(Λ) using the highest-weight contravariant form. It intertwines the CANONICAL module action having the same normalization as projective K0, and sends normalized simple classes to the form-dual projective basis. The KK module action is also sound, but its intertwiner is ΨKK∣β=qdef⁡Λ(β)Ψcan∣β. Thus an unrescaled KK identification is not asserted to send simples to the upper global basis. The Hom pairing is instead first-bar-sesquilinear, h(P,M)=T(P#,M); this does not alter the bilinear tensor-dual identification.

Facts & Assumptions

Given: The standard cyclotomic quotient RΛ, the two Grothendieck groups with their normalizations (Cyclotomic KLR functors define an integrable quantum action on K0 and G0), and the projective identification The cyclotomic projective K0 is the integral highest-weight module.

[F1]

The quotient-cover lemma (Cyclotomic projective covers and dualities descend through the quotient): finite blocks have finitely many absolutely simple graded shift orbits and normalized projective covers; T(P,S)=δP,S in normalized bases and T is A-bilinear with h(P,M)=T(P#,M).

[F2]

The projective identification The cyclotomic projective K0 is the integral highest-weight module: K0(RΛ)≅VA(Λ) with highest vector 1Λ under the vacuum normalization.

Proof

Proof technique: dualize the perfect tensor pairing to an isomorphism onto the restricted weight dual, then check that the adjunction identities of the functors translate into the restricted contravariant-dual action and compare the two normalizations.

1.1F1F2

Perfectness and the dual isomorphism. By [F1] each weight component has finitely many absolutely simple graded shift orbits and normalized projective covers, and the exactness of projective tensor pairing together with the unscaled diagonal values gives perfectness over A on each weight. Hence G0 is free on the simple classes and the functional map Ψcan(M)(ϕ(P))=T(P,M) is an isomorphism from G0(RΛ) to the weightwise dual ⨁βHom⁡A(VA(Λ)Λ−β,A), i.e. the restricted weight dual and not a full unrestricted product dual.

2.1step 1.1F2F3

Intertwining with the canonical action. Transport K0 by ϕ; its tensor form is the actual highest-weight contravariant form with σ(Fi)=qi−1KiEi (The contravariant form on an integrable highest weight module). From tensor adjunction, T(P,FibasicM)=T(EibasicP,M)=T(σ(Fi)P,M), and the analogous normalized identity is T(P,EicanM)=T(σ(Ei)P,M); these are precisely the restricted contravariant-dual action relations, so Ψcan intertwines the canonical module action with the dual action and sends normalized simple classes to the form-dual projective basis.

3.1step 2.1F1F3∎

The KK normalization and the Hom pairing. The Kang--Kashiwara action differs from the canonical one by the weight rescaling qdef⁡Λ(β) on root β, so its intertwiner is ΨKK∣β=qdef⁡Λ(β)Ψcan∣β; in particular the unrescaled KK identification is not asserted to send simples to the upper global basis. The Hom pairing satisfies h(P,M)=T(P#,M) by [F1] and is first-bar-sesquilinear, which concerns the other duality and does not alter the bilinear tensor-dual identification. The Axiom of Choice is inherited only through the integral projective identification [F2] and the contravariant-form suppliers [F3].

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