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LemmaStatement: AI-adaptedProof: AI-adaptedPipeline-generatedprecheck pass
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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.
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Hermitian-reflection and SU(2) QSP convention conversion

Statement

Put s=1−x2, WR=(xss−x), WS=(xisisx), and C=Z(π/4). Then CWRC=iWS†,WS†=Z(π/2)WSZ(−π/2). For d≥1, define US(Ψ)=Z(ψ0)∏j=1d(WSZ(ψj)). If Ψ is the SU(2)-convention phase list with ψ0=ϕ0+π/4, ψj=ϕj−π/2 for 1≤j<d, and ψd=ϕd−3π/4, then UR(Φ)=idUS(Ψ). The affine phase-list map is invertible. The scalar id is part of the identity: in a control-first block diag⁡(I,U) it acts on the active control branch and cannot be discarded as a global phase.

Facts & Assumptions

Given: x∈[−1,1], real phases, and the definitions of WR and Z in QSP signal matrix and ordered phase sequence.

[F1]

QSP signal matrix and ordered phase sequence fixes WR, Z(ϕ), the ordered product, and the control-relevant phase convention.

[F2]

Euler's formula: exp⁡(iθ)=cos⁡θ+isin⁡θ for every real θ gives eiθ=cos⁡θ+isin⁡θ for real θ.

[F3]
[F4]

Real and imaginary parts, complex conjugation, and modulus: conjugation fixes real numbers and sends i to −i.

[F5]

Controlled Unitary Access: control-first access to a two-dimensional target has block matrix diag⁡(I2,U) when that controlled call is explicitly supplied.

[F6]

Quarter-turn values and shifts by pi/2 and pi gives sin⁡(π/2)=1 and cos⁡(π/2)=0; together with [F2], these give eiπ/2=i and e−iπ/2=−i.

Proof

1.1F1F2F3F4F6algebra

By [F2, F6], eiπ/2=i, and [F3] gives eiπ/4e−iπ/4=1. Multiplying the three matrices entry by entry therefore gives CWRC=(ixssix)=iWS†, since [F4] gives WS†=(x−is−isx).

1.2F1F2F3F4F6algebra

By [F2, F6], the diagonal entries of Z(π/2) and Z(−π/2) are i,−i and −i,i, respectively. Multiplication gives Z(π/2)WSZ(−π/2)=(x−is−isx)=WS†.

2.1F1F3step 1.1step 1.2algebra

Rearranging step 1.1 yields WR=iZ(−π/4)WS†Z(−π/4). Substitution in each signal factor and combination of adjacent diagonal phases by [F3] gives UR(Φ)=idZ(ϕ0−π/4)∏j=1d−1(WS†Z(ϕj−π/2))WS†Z(ϕd−π/4).

3.1step 1.2step 2.1algebra

Replacing each WS† by the right side of step 1.2 adds π/2 to the initial phase, leaves each intermediate phase unchanged after its two adjacent shifts cancel, and subtracts π/2 from the final phase. The resulting SU(2) list is exactly the stated Ψ, and the scalar remains id. Each phase shift is affine with coefficient 1, so the map and its inverse are bijections on Rd+1.

4.1F1F5step 3.1algebra∎

When the operation model explicitly supplies the controlled call on a control-first qubit and two-dimensional target, [F5] gives C(US)=diag⁡(I2,US). Substituting idUS on the active branch gives diag⁡(I2,idUS), which differs from iddiag⁡(I2,US) unless id=1, because the inactive block remains I2. Thus id is a relative phase under control and must be retained.

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