Alphabeta Math
LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedjudge pass (gpt-6-luna)
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.

Graph-state stabilizer generators

Statement

Let G=(V,E) be an ordered finite simple graph and let ∣G⟩ be its graph state. Write Xv,Zv for the one-qubit Pauli matrices embedded on the tensor factor indexed by v; in the phase-aware Pauli convention, vertex at zero-based position r is wire r+1. For v∈V, put Kv:=Xv∏u∈N(v)Zu. Each Kv is a Hermitian involution, Kv∣G⟩=∣G⟩, the generators commute pairwise, and their binary Pauli labels are independent. This includes V=∅, where the generating family is empty.

Facts & Assumptions

Given: A finite simple graph G=(V,E), its ordered graph state, and the one-qubit Pauli matrices.

[F1]

The graph state is UG∣+⟩⊗V with one CZuv per edge, and the embedded edge gates commute (Graph state of an ordered finite simple graph, Controlled-Z edge gates commute).

[F2]

The angle-π controlled phase is the diagonal Hermitian involution diag⁡(1,1,1,−1) (Controlled Phase Rotation).

[F3]

Number coordinates by the vertices in their fixed order; ev is the coordinate unit vector at vertex v, and (A2(G))uv=1 exactly when {u,v}∈E. The binary dot product is the coordinate sum ∑w∈Vawbw in F2. Thus A2(G) is symmetric with zero diagonal (Binary adjacency matrix of an ordered finite simple graph).

[F4]

The one-qubit X,Y,Z matrices are Hermitian involutions, and the phase-aware tensor Pauli frame has binary X- and Z-support with zero-scalar convention XxZz (The Pauli matrices, Phase aware n qubit pauli group).

[F5]

Pauli operators commute exactly when their binary labels have zero symplectic pairing (Pauli commutator is symplectic pairing).

Proof

1.1F1F2F3algebra

Every CZuv is a diagonal Hermitian involution by [F2]. Conjugating Xv by an incident gate gives CZuvXvCZuv=ZuXv by checking the four computational-basis pairs; a nonincident edge gate commutes with Xv. Since the edge gates commute by [F1], UGXvUG†=Xv∏u∈N(v)Zu=Kv. The tensor factors are Hermitian involutions, so Kv is also a Hermitian involution.

1.2F3F4F5algebra

The binary label of Kv is (ev,A2(G)ev) because the Z coordinate at u is (A2(G)ev)u=(A2(G))uv. For distinct v,w, the binary symplectic pairing of these labels is ev⋅A2(G)ew+A2(G)ev⋅ew=(A2(G))vw+(A2(G))wv=0 in F2 by [F3]. Thus [F5] gives pairwise commutation. Equivalently, when {v,w}∈E the two local X/Z anticommutations cancel, and when it is not an edge all overlapping factors are both Z or act on different sites.

2.1step 1.1F1algebra

Using Xv∣+⟩⊗V=∣+⟩⊗V and UG†=UG, we obtain Kv∣G⟩=UGXvUG†UG∣+⟩⊗V=UG∣+⟩⊗V=∣G⟩.

3.1F4algebra∎

In a product of generators indexed by S⊆V, the binary X-support is ∑v∈Sev=1S by [F4]. It vanishes only for S=∅, so no nonempty product has identity binary label; the generators are independent. For empty V this assertion is vacuous.

Depends on

Used by

Dependency tree · two levels

27 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