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.
Zero quadratic invariants need not mean flatness
Statement refuted
For every smooth source-free geometric electrovac datum, if , the scalar curvature , , and all vanish, then and the metric is flat, meaning its Riemann tensor vanishes identically as fixed in Null wave curvature and zero quadratic invariants.
Facts & Assumptions
Given: The smooth null-wave electrovac family and its quadratic invariants.
Smooth null electrovac wave candidate data defines the candidate data on from smooth profiles and a transverse harmonic function .
Geometric electrovac equations and flux normalization defines the source-free Einstein-Maxwell equations and curvature convention.
Exact electrovac plane-wave family proves the defined family is a source-free geometric electrovac.
Null wave curvature and zero quadratic invariants proves the four scalar invariants in the Statement vanish identically and gives in the defined coordinates.
Null wave curvature and zero quadratic invariants fixes “flat” to mean that the Riemann tensor vanishes identically on the four-manifold.
Fix a constant with inverse-length units, and set , , and .
Counterexample
The choices in [A1] satisfy the smoothness and transverse-harmonic hypotheses in [F1]. They give and , which is nonzero. Under the definition in [F2], [F3] proves this is a smooth source-free geometric electrovac datum.
Applying [F4] gives . For the constant profile in [A1], [F3] also gives . But , so . Thus the field and Ricci tensor are nonzero and, by [F5], the metric is not flat although all four displayed scalar invariants vanish.