How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Finite/formal gauge covariance and matrix Ward identity
Statement
Let and be the finite-dimensional formal matrices of Finite matrix formal kernel and inverse series, with , invertible, and both coefficient matrices covariant under the vertex phase angles of Finite-graph U(1) phases for matrix kernels. Then is a two-sided inverse of in , and coefficientwise. For a real vertex tuple , put , , and . Write and , and define and coefficientwise along this differentiable phase path. The variations satisfy For ordinary finite matrices , the corresponding resolvent identity is . These are formal or finite algebraic statements; they assert no convergence of a perturbation series, continuum limit, or loop Ward identity.
Facts & Assumptions
Given: , an invertible finite base , link matrices , the phase action , covariance of both coefficient matrices, and the coefficientwise formal-series operations.
The coefficient matrices are covariant for every vertex phase angle; along the path , they vary differentiably by conjugation. The base is invertible. These are hypotheses of the Statement, not conclusions of the proof.
Finite matrix formal kernel and inverse series: and are defined in the formal power-series ring ; each coefficient of is a finite matrix.
Finite-graph U(1) phases for matrix kernels: and ; the hopping blocks are .
Charged gauge data and SI-natural conventions: the continuum charged-field phase is . The finite graph angle of [F2] is independent; identifying it numerically with 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
Put . The coefficient of in is , a finite matrix, so the series defines an element of without an analytic convergence assumption.
Each link block transforms as ; summing links in each block gives . With [A1], the assumed covariance of gives the same conjugation for each coefficient of ; [F3] supplies the separate continuum phase convention, without identifying graph vertices with spacetime points.
Since , multiplication gives . In the product , the constant coefficient is and the two contributions to every positive-degree coefficient cancel; hence .
Also , so by the same coefficientwise cancellation. Thus is the two-sided formal inverse.
Substituting the conjugated into the defining series for conjugates each finite coefficient by , proving .
Use the path , and the definitions of in the Statement. Differentiate coefficientwise at . This gives , hence using .
From , direct differentiation gives . Therefore .
For ordinary invertible finite matrices , expand the product: . This is exactly the resolvent identity in the Statement.