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.
The occupied spectral projector has no continuous extension through a zero gap
Example
For , let . For every the lowest eigenvalue is simple, so its occupied projector is defined; at the occupied/unoccupied gap vanishes and the lowest rank-one projector is not unique. The two one-sided limits of the defined projectors differ.
Facts & Assumptions
Given: The Hermitian path and the rank-one lowest-eigenvalue projector when the gap is positive.
The occupied projector is uniquely defined only on a domain with a strict th gap (The occupied-projector response map on its strict-gap domain).
Verification
If , then and the lowest eigenvector is , so . If , then and the lowest eigenvector is , so .
At , both eigenvalues equal , so the gap is and every rank-one orthogonal projector onto a line is a lowest-eigenspace projector; there is no unique under [F1].
The limits as and are respectively and , which are distinct because their Frobenius distance is . Thus no continuous extension of the uniquely gapped projector exists at .
Depends on
Used by
Nothing in the library uses this result yet.
Dependency tree · two levels
3 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Tosio Kato, Perturbation Theory for Linear Operators, 2nd ed., Chapter II §1.4–§1.6 (standard reference, not scraped)