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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedverified 2026-10-15 (gpt-6-luna, gpt-6.1-sol, and delegated Codex review/repair agents; see completed run evidence)
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Finite/formal gauge covariance and matrix Ward identity

Statement

Let K(z;ζ)=K0(ζ)+zV(ζ) and S(z;ζ) be the finite-dimensional formal matrices of Finite matrix formal kernel and inverse series, with d≥1, K0(ζ) invertible, and both coefficient matrices covariant under the vertex phase angles of Finite-graph U(1) phases for matrix kernels. Then S is a two-sided inverse of K in Md(C⟦z⟧), and S(z;ζθ)=DθS(z;ζ)Dθ−1 coefficientwise. For a real vertex tuple θ, put Θ:=diag⁡x∈X(θxIr), ζs:=ζsθ, and Ds:=Dsθ=eisΘ. Write Ks:=K(z;ζs) and Ss:=S(z;ζs), and define δK:=ddsKs∣s=0 and δS:=ddsSs∣s=0 coefficientwise along this differentiable phase path. The variations satisfy δK=i[Θ,K],δS=i[Θ,S]=−S(δK)S. For ordinary finite matrices A,B∈GLd(C), the corresponding resolvent identity is B−1(B−A)A−1=A−1−B−1. These are formal or finite algebraic statements; they assert no convergence of a perturbation series, continuum limit, or loop Ward identity.

Facts & Assumptions

Given: d≥1, an invertible finite base K0, link matrices V(ζ), the phase action Dθ, covariance of both coefficient matrices, and the coefficientwise formal-series operations.

[A1]

The coefficient matrices are covariant for every vertex phase angle; along the path θ(s)=sθ, they vary differentiably by conjugation. The base is invertible. These are hypotheses of the Statement, not conclusions of the proof.

[F1]

Finite matrix formal kernel and inverse series: K=K0+zV and S=∑n≥0(−zK0−1V)nK0−1 are defined in the formal power-series ring C⟦z⟧; each coefficient of S is a finite matrix.

[F2]

Finite-graph U(1) phases for matrix kernels: ζeθ=ei(θs(e)−θt(e))ζe and Dθ=diag⁡x(eiθxIr); the hopping blocks are Teζe.

[F3]

Charged gauge data and SI-natural conventions: the continuum charged-field phase is eigα(x). The finite graph angle of [F2] is independent; identifying it numerically with gαx requires a separately assigned real vertex tuple and does not choose a spacetime embedding. This convention is distinct from the phase action used by the finite algebraic proof.

Proof

1.1givenF1algebra

Put B:=K0−1V. The coefficient of zn in S is (−B)nK0−1, a finite matrix, so the series defines an element of Md(C⟦z⟧) without an analytic convergence assumption.

1.2A1F1F2F3algebra

Each link block transforms as Teζeθ=eiθs(e)(Teζe)e−iθt(e); summing links in each block gives V(ζθ)=DθV(ζ)Dθ−1. With [A1], the assumed covariance of K0 gives the same conjugation for each coefficient of K; [F3] supplies the separate continuum phase convention, without identifying graph vertices with spacetime points.

2.1A1F1step 1.1algebra

Since K=K0(I+zB), multiplication gives KS=K0(I+zB)∑n≥0(−zB)nK0−1. In the product (I+zB)∑n≥0(−zB)n, the constant coefficient is I and the two contributions to every positive-degree coefficient cancel; hence KS=I.

2.2A1F1step 1.1algebra

Also K0−1K=I+zB, so SK=∑n≥0(−zB)n(I+zB)=I by the same coefficientwise cancellation. Thus S is the two-sided formal inverse.

2.3F1step 1.2algebra

Substituting the conjugated K0,V into the defining series for S conjugates each finite coefficient by Dθ, proving S(z;ζθ)=DθS(z;ζ)Dθ−1.

3.1F1F2step 2.1step 2.2givenalgebra

Use the path ζs=ζsθ, Ds=Dsθ and the definitions of Ks,Ss,δ in the Statement. Differentiate KsSs=I coefficientwise at s=0. This gives (δK)S+K(δS)=0, hence δS=−S(δK)S using K−1=S.

4.1A1step 2.1step 2.2step 3.1givenalgebra

From Ds=eisΘ, direct differentiation gives δK=i[Θ,K]. Therefore −S i[Θ,K] S=−iSΘKS+iSKΘS=−iSΘ+iΘS=i[Θ,S].

5.1givenalgebra∎

For ordinary invertible finite matrices A,B, expand the product: B−1(B−A)A−1=B−1BA−1−B−1AA−1=A−1−B−1. This is exactly the resolvent identity in the Statement.

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