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CNOT Pauli action

Statement

Let n≥2 and let distinct c,t∈{1,…,n} be control and target indices. For CNOT Cc→t acting on y∈F2n by toggling coordinate t by yc, conjugation sends

P(k,x,z)⟼P(k,x′,z′),xt′=xt+xc,zc′=zc+zt,

with all other coordinates unchanged and additions in F2. In particular, Xc↦XcXt, Zc↦Zc, Xt↦Xt, and Zt↦ZcZt; the phase coordinate k is unchanged in the fixed XxZz order.

Facts & Assumptions

Given: n≥2, distinct control and target wires c,t∈{1,…,n}, the ordered computational basis, and the phase-aware Pauli convention.

[F1]

The Pauli matrices: X flips a one-bit computational basis vector and Z multiplies it by (-1)^b.

[F2]

Pauli matrix algebra and trace identities: X and Z are Hermitian involutions.

[F3]

Controlled Unitary Access: controlled access has control-first block form C(U)=diag(I,U).

[F4]

CNOT and Control-Target Order: on the first two wires, CNOT sends |a,t> to |a,t+a> with first wire control.

[F6]

Ordered tensor registers, their inner product, and wire permutations: a wire permutation is the unique linear extension of the corresponding permutation of ordered product-basis vectors.

Proof

1.1givenF1F2F3F4F5algebra

For control c=1 and target t=2, the controlled-X definition [F3,F4] gives C∣y1,…,yn⟩=∣y1,…,yt+yc,…,yn⟩. Applying this rule twice gives C2=I; it permutes the ordered orthonormal basis, so C=C∗. On a basis vector, in CXcC the right CNOT first changes yt to yt+yc, the middle Xc changes yc to yc+1, and the left CNOT changes the target to yt+yc+(yc+1)=yt+1. Thus CXcC=XcXt. In CXtC, the right CNOT changes the target to yt+yc, the middle Xt toggles it, and the left CNOT toggles it back by yc, leaving yt+1; hence CXtC=Xt. The middle Zc contributes (−1)yc and the two CNOTs restore the bits, giving CZcC=Zc. The middle Zt contributes (−1)yt+yc, giving CZtC=ZcZt.

2.1givenF4F6step 1.1constructalgebra

For arbitrary distinct wires c,t∈{1,…,n}, assign source positions 0,1 to c−1,t−1. This partial assignment is injective; list its remaining source and target positions in increasing order and match them in order to extend it to a permutation σ. By [F6], Pσ moves those factors into the first two positions and permutes an orthonormal basis bijectively, so Pσ is unitary. The operator Pσ−1(C1→2⊗Iremaining)Pσ therefore has the stated basis action, and its Pauli conjugation rules are the first-two-wire rules of step 1.1 with local wire names 1,2 replaced by c,t.

3.1givenF5step 2.1algebra∎

Write P(k,x,z) as its ordered product of all X-factor maps followed by all Z-factor maps. Conjugation preserves this product order. Using step 2.1, the images of the X factors combine to XcxcXtxt+xc with all other X exponents unchanged; the images of the Z factors combine to Zczc+ztZtzt with all other Z exponents unchanged. Tensor-map composition in [F5] justifies these factorwise products, and no X factor is moved past a Z factor. Thus no scalar is introduced, k is unchanged, and the stated binary updates follow.

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