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ExampleConstruction: AI-generatedVerification: AI-generatedPipeline-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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Charged expectation vanishes by gauge averaging

Example

Take a two-vertex graph with one link e:v1→v2, one fermion mode per vertex and zero backgrounds. The zero-electric, zero-occupation vector Ω is physical. The bounded creation operator O=cv1,1† has nonzero gauge charge at v1, so its expectation in any physical vector, including Ω, vanishes.

Facts & Assumptions

Given: The conditional finite-graph CAR model, the gauge action, and the Axiom of Choice required by the time-dependent Ward supplier.

[A1]

The Axiom of Choice is the principle that every family of nonempty sets has a choice function. The Axiom of Choice

[F1]

Exact regulated gauge and infinitesimal Ward identities: every bounded gauge-charge eigenoperator with nonzero charge has zero expectation in a physical vector; time evolution preserves gauge charge under AC. This current A-page item depends on the still-draft QFT-MF01 CAR supplier through its graph-model dependencies.

Verification

Given: [A1], [F1], and the zero-background two-vertex state described above.

1.1A1F1given

For Ω, nv1=nv2=0 and Ee=0, so both Gauss eigenvalues vanish. The CAR creation operator is bounded and nonzero; the gauge law gives U(α)OU(α)†=e−iαv1O, so its charge vector is qv1=−1,qv2=0.

2.1F1step 1.1algebra∎

The nonzero charge in step 1.1 forces ⟨Ω,OΩ⟩=0 by the finite-regulator selection rule, even though OΩ is a nonzero one-fermion vector. This demonstrates that the selection rule concerns expectations in the physical sector, not the vanishing of the charged operator itself.

Depends on

Dependency tree · 2 levels

Sources