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ExampleConstruction: AI-generatedVerification: AI-generatedPipeline-generatedjudge pass (gpt-6-luna)
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

Physical scope

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 K consist of one vertex and no higher-dimensional simplices in the relative state-sum convention for the finite model with G=Z/2 and A={0}. There is one background object, its first automorphism group has order 2, and its second automorphism group is trivial. The normalized spin partition weight for the unique background is 1, and the normalized background-gauging amplitude is 1/2.

Facts & Assumptions

Given: the one-vertex boundary complex and the adopted normalized spin model.

[F1]

Finite two-group lattice spin state-sum model: spin configurations are vertex labels in Z/2, each of weight 2−V; the background gauge group has G=Z/2 and trivial A.

[F2]

Gauge invariance and gluing in the finite symmetry model: the background amplitude is the higher sum with component mass ∣π2∣/∣π1∣.

[A1]

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.

1.1givenF1A1algebra

There is one flat background object. Its raw vertex gauge labels are G=Z/2 and its 2-gauge group is A={0}, so ∣π1∣=2 and ∣π2∣=1. The two spin assignments each have weight 1/2, hence their total per-background partition weight is 1.

2.1givenA1F2step 1.1algebra∎

Under the adopted model the sole background component contributes 1⋅∣π2∣/∣π1∣=1/2 to the finite gauging sum.

Depends on

Dependency tree · 2 levels