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.
Allowed and excluded order-two forward coefficients
Example
At truncation order , let denote the normalized forward on-shell amplitude coordinates and let be the finite feasible set defined by the order-two constraints. The strict region is contained in . The strict region is disjoint from . The vectors and witness that both regions are nonempty. The first region passes the finite necessary test; this example does not assert that any vector passing that test extends to full analytic amplitude data or a physical theory, and it assigns no sign to a generic off-shell Lagrangian coefficient.
Example references
Facts & Assumptions
Given: The normalized on-shell coordinates , the definition of , and the finite-constraint proposition.
Finite truncated forward-amplitude bootstrap data: for , the applicable constraints are , , , and .
Finite truncated forward-positivity constraints: every amplitude-data vector under the stated gapped-scalar hypotheses lies in .
Verification
For any , the order-one Hankel quadratic form is , which is positive for every nonzero because and . The remaining order-two inequalities are , , and by [F1]; hence . For , the order-one determinant is , while , , and are positive, so it lies in .
For any , choose . Its order-one Hankel quadratic form equals , so that matrix is not positive semidefinite and . In particular, for this vector is and the value is .
By [F2], any coefficient vector arising from the specified gapped amplitude data must satisfy every order-two constraint. Hence is excluded under those hypotheses, while the finite test alone only labels as allowed by ; it supplies no converse or physical realization.