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Affine current fields are local with the normalized current OPE

Statement

Let Vk(g) be the vacuum module of Universal affine vacuum module, with g finite-dimensional complex simple and k∈C. Then for every x∈g, Jx(z)=∑n∈Zxnz−n−1 is a field, is creative with Jx(z)1=ezT(x−11), and is translation-covariant. For x,y∈g, [Jx(z),Jy(w)]=J[x,y](w)δ(z,w)+kB(x,y)∂wδ(z,w), so the current fields are pairwise local of order at most 2, with formal OPE Jx(z)Jy(w)∼J[x,y](w)z−w+kB(x,y)id⁡(z−w)2.

Facts & Assumptions

Given: The simple Lie algebra, normalized invariant form, level k, and induced vacuum module.

[F1]

Universal affine vacuum module: the central generator acts as k and g[t] kills 1.

[F2]

The universal affine vacuum module is restricted: all sufficiently large positive modes of a fixed current kill each fixed vector of Vk(g).

[F3]

Mode translation descends to the affine vacuum module: T1=0 and [T,xn]=−nxn−1.

[F4]

Untwisted affine central extension: [xm,yn]=[x,y]m+n+mδm,−nB(x,y)K.

[F5]

Locality determines the formal OPE coefficients: δ(z,w)=∑m∈Zz−m−1wm, (z−w)δ=0, and (z−w)2∂wδ=0; its locality expansion identifies the formal OPE coefficients.

Proof

1.1F1F2F3algebra

By [F2], for each vector v the modes xnv vanish for sufficiently large n, so Jx(z) is a field. By [F1], xn1=0 for n≥0, whence Jx(z)1=∑r≥0x−r−11 zr. From [F3], induction gives Trx−11=r!x−r−11: the induction step is Tx−r−11=(r+1)x−r−21. Thus the displayed series is ezT(x−11). The same relation gives [T,Jx(z)]=∑n(−n)xn−1z−n−1=∂zJx(z) after the index change m=n−1.

2.1F1F4F5step 1.1algebra

By [F4] and the scalar action of K in [F1], [Jx(z),Jy(w)]=∑m,n[xm,yn]z−m−1w−n−1. For the loop term set r=m+n; it becomes J[x,y](w)∑mz−m−1wm=J[x,y](w)δ(z,w). The central term is kB(x,y)∑mmz−m−1wm−1=kB(x,y)∂wδ(z,w). Both reindexings are coefficient identities of formal distributions; each coefficient in the two-variable series is a finite sum.

3.1F5step 2.1algebra∎

Multiplying the commutator in step 2.1 by (z−w)2 gives zero: (z−w)δ=0 and differentiating it gives (z−w)∂wδ=δ, hence (z−w)2∂wδ=0. This proves locality. The coefficient formula in [F5] gives the two singular coefficients J[x,y] and kB(x,y)id⁡ and no higher ones, yielding the displayed OPE.

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