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The categorical sl2 commutator in a small cyclotomic weight

Example

Take I={i} with (αi∣αi)=2, di=1, qi=q, and Λ=2Λ1, so that ⟨hi,Λ⟩=2 and the standard cyclotomic quotient has relations x12e(ν)=0. Then:

(a) RΛ(0)=k, RΛ(αi)=k[x1]/(x12) with graded dimension 1+q2, and RΛ(nαi)=0 for n≥3, so the functors on the nonzero weights are FiΛk=RΛ(αi) and FiΛEiΛk=0;

(b) the categorical sl2 relation of The categorical sl2 commutator for cyclotomic KLR functors at β=0, λ=Λ (case ⟨hi,λ⟩=2≥0) reads q−2FiΛEiΛ⊕Id⊕q2Id≅EiΛFiΛ; on the vacuum it says EiΛFiΛk≅k⊕k{2}, which is exactly RΛ(αi)≅k⊕k{2};

(c) consequently, with the normalized operators of Cyclotomic KLR functors define an integrable quantum action on K0 and G0, on [Proj(RΛ(0))]: EiFi[1Λ]=(q+q−1)[1Λ] and FiEi[1Λ]=0, so [Ei,Fi][1Λ]=(q+q−1)[1Λ]=(Ki−Ki−1)/(qi−qi−1)[1Λ] with Ki[1Λ]=q2[1Λ]; on [Rep(RΛ(0))] the same commutator identity holds: Fi[k]=q−1[k⊕k{2}], Ei lowers back, FiEi[k]=0, and EiFi[k]=(q+q−1)[k]. This is the mixed relation of Cyclotomic KLR functors define an integrable quantum action on K0 and G0 verified at the first nontrivial weight.

Verification

Given: The rank-one datum I={i}, (αi∣αi)=2, di=1, qi=q, Λ=2Λ1, with the standard quotient x12e(ν)=0 and the functors of Cyclotomic KLR induction and restriction functors.

[F1] The rank-one quotients: RΛ(0)=k, RΛ(αi)=k[x]/(x2) of graded dimension 1+q2, RΛ(nαi)=0 for n≥3, and basic restriction of Fik is the vector space k⊕k{2} (Cyclotomic KLR quotients in ranks zero, one and two).

[F2] The categorical sl2 relation at target weight h=2 has identity shifts 0,2, so its vacuum evaluation is exactly k⊕k{2} (The categorical sl2 commutator for cyclotomic KLR functors).

[F3] The normalized operators on K0 carry q−1 on projective E at input root αi, while KK module F carries q−1 and KK E is raw, and the canonical module action shifts E and leaves F raw (Cyclotomic KLR functors define an integrable quantum action on K0 and G0).

Verification.

1.1F1

The blocks. The rank-zero block is k and the rank-one quotient is k[x]/(x2) with basis 1,x and degrees 0,2. Restriction of the vacuum has zero target. Thus the relevant functor values on the vacuum are FiΛk=RΛ(αi) and FiΛEiΛk=0.

2.1step 1.1F2

The commutator. The relation of [F2] evaluated on the vacuum gives EiΛFiΛk≅k⊕k{2}, which is RΛ(αi) by [F1], so q−2FiΛEiΛ⊕Id⊕q2Id≅EiΛFiΛ holds at the first nontrivial weight.

3.1step 2.1F3∎

The Grothendieck commutator. With the normalizations of [F3]: projective EiFi[1Λ]=q−1(1+q2)[1Λ]=(q+q−1)[1Λ] and FiEi[1Λ]=0; KK module F from the vacuum also carries q−1 while KK E is raw, and the canonical module action shifts E and leaves F raw, giving the same result in both module conventions. All agree with (q2−q−2)/(q−q−1), the mixed relation evaluated at Ki=q2. This verifies the commutator identity at the first nontrivial weight and is a finite rank-one computation using no choice.

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