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.
Controlled-Z matching action on a Pauli frame
Statement
Let and let be a matching, meaning a set of pairwise disjoint two-element subsets of the ordered wire set . Give the graph the vertex order , so vertex is coordinate (position in the zero-based vertex list) of its binary adjacency matrix. Let from Binary adjacency matrix of an ordered finite simple graph, so exactly when . For , all coordinates use this wire order, and binary dot products mean in . Define . For , put as in Phase aware n qubit pauli group. For , the unique empty vectors satisfy and we define ; the register is the empty tensor product from Ordered tensor registers, their inner product, and wire permutations. With ,
For the empty wire set or empty matching the sum is zero and the formula is the identity.
Facts & Assumptions
Given: A finite ordered set of qubits, a matching , and binary vectors .
The angle- controlled phase acts on by (Controlled Phase Rotation).
is symmetric with zero diagonal and records precisely the matching edges (Binary adjacency matrix of an ordered finite simple graph).
For , the Pauli frame convention is on the ordered register (Phase aware n qubit pauli group). The identity convention is specified in the Statement.
The zero-wire tensor register is with basis , and the product basis spans each finite ordered register (Ordered tensor registers, their inner product, and wire permutations).
Proof
For , write . By [F1], . Expanding each edge term over gives the cross term . By the stated coordinate order and dot-product convention, , so this cross term is exactly . Hence .
Applying the left side of the claimed identity to gives . Applying the right side gives ; step 1.1 makes these signs equal. The ordered computational basis spans the register, so the operators agree. When or , every sum is empty and both sides are the identity frame relation by [F3]--[F4].
Depends on
Used by
Dependency tree · two levels
31 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
- Ronald de Wolf, Quantum Computing: Lecture Notes, arXiv:1907.09415, §20.6 (standard reference, not scraped)
- Robert Raussendorf, Daniel E. Browne, and Hans J. Briegel, Measurement-based quantum computation on cluster states, §II B (standard reference, not scraped)