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The A1 Nakajima Hecke correspondence gives the fundamental sl2 action

Statement

Use A one-vertex framed quiver variety and its Hecke correspondence and The A1 Nakajima varieties and the Hecke correspondence are points. Let ev be the fundamental class of L(v,1) in H0(L(v,1);C), for v=0,1. Define F by the P0,1 correspondence only from the v=0 summand to the v=1 summand, and extend it by zero on v=1. Define E by the reverse correspondence, with Nakajima's sign (−1)(d(0,1)−d(1,1))/2, only from v=1 to v=0, and extend it by zero on v=0, where d(v,1)=dim⁡CM(v,1). The preceding lemma says both dimensions are zero, so this coefficient is 1. Let H act on the v-summand by 1−2v. Then Ee0=0,Ee1=e0,Fe0=e1,Fe1=0,He0=e0,He1=−e1. These operators define the standard two-dimensional representation of sl2(C), the trace-zero 2×2 matrices with commutator bracket.

Facts & Assumptions

Given: The framed A1 data, its correspondence, and the point classes specified in the Statement.

[F1]

A one-vertex framed quiver variety and its Hecke correspondence: when P0,1 and both spaces are points and the projections are identities, its fundamental-class correspondence map sends the source point class to the target point class; the reverse map uses the same rule.

[F2]

The A1 Nakajima varieties and the Hecke correspondence are points: L(0,1), L(1,1) and P0,1 are points, and each projection of P0,1 is the identity map.

Proof

1.1givenF1F2F4algebra

By [F2] and [F4], each summand is one-dimensional with its point class as basis, and each point has complex dimension zero. The projections of P0,1 are identities; hence [F1]'s point correspondence rule sends e0 to e1 and its reverse sends e1 to e0. The reverse sign is (−1)(0−0)/2=1; extending the maps by zero on the other summands gives the stated actions.

2.1F1step 1.1algebra

On e0, EFe0=e0 and FEe0=0; on e1, EFe1=0 and FEe1=e1. Thus [E,F] has eigenvalues 1,−1 on e0,e1, respectively, which are the specified H-weights, so [E,F]=H.

2.2F1step 1.1algebra

On e0, [H,E]e0=H(0)−E(e0)=0=2Ee0; on e1, [H,E]e1=H(e0)−E(−e1)=2e0=2Ee1. Hence [H,E]=2E.

3.1F1step 1.1algebra∎

On e1, [H,F]e1=H(0)−F(−e1)=0=−2Fe1; on e0, [H,F]e0=H(e1)−F(e0)=−2e1=−2Fe0. Hence [H,F]=−2F. In the ordered basis (e0,e1) these actions are E=(0100), F=(0010), and H=(100−1); their brackets just verified are the defining brackets of the trace-zero matrix Lie algebra, so the action is its standard representation.

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