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.
Point normalization in the finite symmetry model
One-vertex boundary evaluation in the adopted finite G = Z/2 model with trivial A and normalized spin measure; no continuum or empirical claim.
Example
Let consist of one vertex and no higher-dimensional simplices in the relative state-sum convention for the finite model with and . There is one background object, its first automorphism group has order , and its second automorphism group is trivial. The normalized spin partition weight for the unique background is , and the normalized background-gauging amplitude is .
Example references
Facts & Assumptions
Given: the one-vertex boundary complex and the adopted normalized spin model.
Finite two-group lattice spin state-sum model: spin configurations are vertex labels in , each of weight ; the background gauge group has and trivial .
Gauge invariance and gluing in the finite symmetry model: the background amplitude is the higher sum with component mass .
Adopted finite two-group gauging model: the finite spin model and unit background response are adopted assumptions.
Verification
Given: one vertex, no edges, and no face labels.
There is one flat background object. Its raw vertex gauge labels are and its -gauge group is , so and . The two spin assignments each have weight , hence their total per-background partition weight is .
Under the adopted model the sole background component contributes to the finite gauging sum.