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LemmaStatement: AI-adaptedProof: AI-adaptedPipeline-generatedjudge pass (gpt-6-luna)
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Controlled-Z matching action on a Pauli frame

Statement

Let n≥0 and let M be a matching, meaning a set of pairwise disjoint two-element subsets of the ordered wire set {1,…,n}. Give the graph GM=({1,…,n},M) the vertex order 1,…,n, so vertex j is coordinate j (position j−1 in the zero-based vertex list) of its binary adjacency matrix. Let AM:=A2(GM)∈Mn(F2) from Binary adjacency matrix of an ordered finite simple graph, so (AM)jk=1 exactly when {j,k}∈M. For x,z∈F2n, all coordinates use this wire order, and binary dot products mean a⋅b:=∑j=1najbj in F2. Define qM(x):=∑{j,k}∈Mxjxk∈F2. For n≥1, put P(x,z):=XxZz=P(0,x,z) as in Phase aware n qubit pauli group. For n=0, the unique empty vectors satisfy Xx=Zz=IC and we define P(x,z)=IC; the register is the empty tensor product from Ordered tensor registers, their inner product, and wire permutations. With CZM:=∏{j,k}∈MCZjk,

CZMP(x,z)=(−1)qM(x)P(x,z⊕AMx)CZM.

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 n qubits, a matching M, and binary vectors x,z∈F2n.

[F1]

The angle-π controlled phase acts on ∣yjyk⟩ by (−1)yjyk (Controlled Phase Rotation).

[F2]

AM is symmetric with zero diagonal and records precisely the matching edges (Binary adjacency matrix of an ordered finite simple graph).

[F3]

For n≥1, the Pauli frame convention is P(x,z)=P(0,x,z)=XxZz on the ordered register (Phase aware n qubit pauli group). The n=0 identity convention is specified in the Statement.

[F4]

The zero-wire tensor register is C with basis {1}, and the product basis spans each finite ordered register (Ordered tensor registers, their inner product, and wire permutations).

Proof

1.1F1F2algebra

For y∈F2n, write qM(y)=∑{j,k}∈Myjyk. By [F1], CZM∣y⟩=(−1)qM(y)∣y⟩. Expanding each edge term over F2 gives the cross term ∑{j,k}∈M(yjxk+xjyk). By the stated coordinate order and dot-product convention, (AMx)j=∑k:{j,k}∈Mxk, so this cross term is exactly (AMx)⋅y. Hence qM(y⊕x)=qM(y)+qM(x)+(AMx)⋅y.

2.1step 1.1F3F4algebracases∎

Applying the left side of the claimed identity to ∣y⟩ gives (−1)z⋅y+qM(y⊕x)∣y⊕x⟩. Applying the right side gives (−1)qM(x)+qM(y)+(z⊕AMx)⋅y∣y⊕x⟩; step 1.1 makes these signs equal. The ordered computational basis spans the register, so the operators agree. When n=0 or M=∅, every sum is empty and both sides are the identity frame relation by [F3]--[F4].

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