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Formal coordinate-change action of a conformal vertex algebra

Statement

Let V=⨁m≥0Vm be a conformal vertex algebra of CFT type over C, with the Virasoro operators fixed in the corresponding Definition. Let ρ(t)=a1exp⁡(∑n>0cntn+1∂t)t be a holomorphic germ at 0 with a1≠0. The formal-coordinate operator on V is

U(ρ)=a1L(0)exp⁡ ⁣(∑n>0cnL(n)).

On each finite weight truncation V≤d=⨁0≤m≤dVm, the exponential is a finite sum on each vector because each L(n) with n>0 lowers L(0)-weight. These operators satisfy U(ρ1∘ρ2)=U(ρ1)U(ρ2) and are invertible. If ρ varies holomorphically with a parameter, the restrictions of U(ρ) to each V≤d vary holomorphically.

Facts & Assumptions

[F1]

The grading, finite-dimensional weight spaces, and Virasoro brackets are those of Conformal vertex algebra of CFT type, Vertex algebra in the state–field convention and Virasoro algebra in the Lm convention.

[F2]

The positive-mode exponential is a polynomial representation of tangent-to-identity finite jets, compatible with weight restrictions, by Finite-jet integration of positive Virasoro operators.

Proof

Given: The algebra V and germs in the statement. Write sa(t)=at and let Gd denote the tangent-to-identity jets modulo td+2.

1.1F1F2constructalgebra

Every germ has a unique formal factorization ρ=sa∘f, with a=ρ′(0)≠0 and f′(0)=1. At each jet order the triangular recursion of [F2] gives the unique coefficients c1,…,cd in f=exp⁡(∑cntn+1∂t)t. The recursions are compatible as d increases; this establishes the infinite formal expression. It does not assert that its logarithmic vector field converges as a holomorphic vector field. On Ed=V≤d each mode with n>d vanishes and every product of more than d positive modes vanishes. Hence the displayed operator is well-defined there and equals A(a)Rd(f), where A(a)∣Vm=amI. The finite restrictions agree and therefore define an operator on the algebraic direct sum V.

2.1step 1.1F2algebra

For b≠0 put f[b]=sb−1∘f∘sb. Conjugation changes tn+1∂t to bntn+1∂t in the exponential expression for f[b]. Weight lowering gives A(b)−1L(n)A(b)=bnL(n), so Rd(f)A(b)=A(b)Rd(f[b]). If ρ1=sa∘f and ρ2=sb∘g, their composite is sab∘f[b]∘g. Applying [F2] and this conjugation identity gives U(ρ1)U(ρ2)=A(ab)Rd(f[b])Rd(g)=U(ρ1∘ρ2) on Ed. Compatibility proves the identity on V. Since U(id)=I and a germ with nonzero derivative has an inverse germ, U(ρ−1) is the two-sided inverse. Alternatively invertibility on each jet follows from the finite polynomial inverse and A(a)−1=A(a−1).

3.1step 1.1step 2.1F1F2∎

For a holomorphic family of germs, every Taylor coefficient and the nonvanishing derivative a are holomorphic in the parameter. Division by a gives holomorphic coefficients of f, and the finite triangular recursion makes every cn holomorphic. On Ed the finite exponential is polynomial in c1,…,cd and A(a) has entries am, 0≤m≤d. Thus every matrix entry is holomorphic. No branch of log⁡a is needed because the weights are integers. This proves all the assertions.

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