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Adjacent Gaussian gates are exactly special-unitary parity blocks, with common phases separated

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QAlgorithms.Papers.Independent.Intakethird100.P77.nearestNeighbour_gaussianIdentification

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Fix an existing adjacent pair of wires in increasing order in the Jordan–Wigner representation. Let G\mathcal GG be the set of operators eiHe^{iH}eiH, with H=i∑μ≠νhμνcμcνH=i\sum_{\mu\ne\nu}h_{\mu\nu}c_\mu c_\nuH=i∑μ=ν​hμν​cμ​cν​, real antisymmetric hhh, and all coefficients outside the four Majoranas of that pair equal to zero. Then

G={G(A,B):A,B∈SU(2)},{G(A,B):A,B∈U(2),det⁡A=det⁡B}={zV:∣z∣=1, V∈G}.\mathcal G=\{G(A,B):A,B\in SU(2)\},\qquad \{G(A,B):A,B\in U(2),\det A=\det B\}=\{zV:|z|=1,\ V\in\mathcal G\}.G={G(A,B):A,B∈SU(2)},{G(A,B):A,B∈U(2),detA=detB}={zV:∣z∣=1, V∈G}.

All operators are embedded on the specified pair and act as identity elsewhere. The two parity bases are ordered 00,1100,1100,11 and 01,1001,1001,10. This gives the exact local identification while retaining the scalar phase needed for general allowable matchgates.

Source correction. The unrestricted equal-determinant assertion on p.11 omits the common scalar phase; the trace-free quadratics themselves generate determinant-one blocks.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P77
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P77

open QAlgorithms

open QAlgorithms.Complexity (Str)

open QAlgorithms.Papers.Independent.Advance50.P19 (Major CARSystem)

open QAlgorithms.Papers.Independent.Information100.P32 (Op)

open scoped BigOperators Matrix ComplexConjugate

attribute [local instance] Classical.propDecidable Classical.decEq

/-- PDF pp.10--11 local identification, with the scalar-phase omission
corrected: trace-free quadratics give exactly determinant-one parity blocks;
general equal-determinant blocks are these times a common unit scalar. -/
theorem nearestNeighbour_gaussianIdentification {n : ℕ} (w : Fin 2 ↪ Fin n)
    (hadjacent : (w 0).val + 1 = (w 1).val) (U : Op (Qubits n)) :
    ((∃ h : Matrix (Major n) (Major n) ℝ,
        Skew h ∧ SupportedOnPair w h ∧ U = gaussianOperation (jordanWigner n) h) ↔
      ∃ A B : Matrix.unitaryGroup Bool ℂ,
        Matrix.det (A : Matrix Bool Bool ℂ) = 1 ∧
        Matrix.det (B : Matrix Bool Bool ℂ) = 1 ∧
        U = embedOp (parityGate A B) w) ∧
    ((∃ A B : Matrix.unitaryGroup Bool ℂ,
        Matrix.det (A : Matrix Bool Bool ℂ) = Matrix.det (B : Matrix Bool Bool ℂ) ∧
        U = embedOp (parityGate A B) w) ↔
      ∃ (z : ℂ) (h : Matrix (Major n) (Major n) ℝ),
        ‖z‖ = 1 ∧ Skew h ∧ SupportedOnPair w h ∧
        U = z • gaussianOperation (jordanWigner n) h) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P77

end
Source
Matchgates and classical simulation of quantum circuits, arXiv:0804.4050v2, PDF p. 11, Section 5: local Gaussian gates and nearest-neighbour matchgates, with phase correction
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every natural number nnn, every injection w:{0,1}↪{0,…,n−1}w:\{0,1\}\hookrightarrow\{0,\ldots,n-1\}w:{0,1}↪{0,…,n−1} satisfying w(1)=w(0)+1w(1)=w(0)+1w(1)=w(0)+1, and every complex matrix UUU indexed by nnn-bit strings, the following two equivalences hold. To specify them, let c2k=Z⊗k⊗X⊗I⊗(n−k−1)c_{2k}=Z^{\otimes k}\otimes X\otimes I^{\otimes(n-k-1)}c2k​=Z⊗k⊗X⊗I⊗(n−k−1) and c2k+1=Z⊗k⊗Y⊗I⊗(n−k−1)c_{2k+1}=Z^{\otimes k}\otimes Y\otimes I^{\otimes(n-k-1)}c2k+1​=Z⊗k⊗Y⊗I⊗(n−k−1), where X=(0110)X=\begin{pmatrix}0&1\\1&0\end{pmatrix}X=(01​10​), Y=(0−ii0)Y=\begin{pmatrix}0&-i\\i&0\end{pmatrix}Y=(0i​−i0​), and Z=diag⁡(1,−1)Z=\operatorname{diag}(1,-1)Z=diag(1,−1), with Boolean indices ordered false, true. For a real 2n×2n2n\times2n2n×2n matrix hhh, set G(h)=exp⁡ ⁣(i[i∑r≠shrscrcs])G(h)=\exp\!\left(i\left[i\sum_{r\ne s}h_{rs}c_rc_s\right]\right)G(h)=exp(i[i∑r=s​hrs​cr​cs​]). The conditions on hhh below are hrs=−hsrh_{rs}=-h_{sr}hrs​=−hsr​ and hrs=0h_{rs}=0hrs​=0 whenever either ⌊r/2⌋\lfloor r/2\rfloor⌊r/2⌋ or ⌊s/2⌋\lfloor s/2\rfloor⌊s/2⌋ lies outside {w(0),w(1)}\{w(0),w(1)\}{w(0),w(1)}. For two Boolean-indexed matrices A,BA,BA,B, define K(A,B)K(A,B)K(A,B) on two-bit strings by setting its (x,y)(x,y)(x,y) entry to zero when x0xorx1≠y0xory1x_0\mathbin{\mathrm{xor}}x_1\ne y_0\mathbin{\mathrm{xor}}y_1x0​xorx1​=y0​xory1​, to Ax0,y0A_{x_0,y_0}Ax0​,y0​​ when both parities are false, and to Bx0,y0B_{x_0,y_0}Bx0​,y0​​ when both are true. Its embedding Ew(K)E_w(K)Ew​(K) has (x,y)(x,y)(x,y) entry K(x∘w,y∘w)K(x\circ w,y\circ w)K(x∘w,y∘w) if xxx and yyy agree on every wire outside the image of www, and zero otherwise. First, there exists an hhh satisfying the stated conditions with U=G(h)U=G(h)U=G(h) if and only if there exist unitary 2×22\times22×2 matrices A,BA,BA,B, each of determinant 111, with U=Ew(K(A,B))U=E_w(K(A,B))U=Ew​(K(A,B)). Second, there exist unitary 2×22\times22×2 matrices A,BA,BA,B with det⁡A=det⁡B\det A=\det BdetA=detB and U=Ew(K(A,B))U=E_w(K(A,B))U=Ew​(K(A,B)) if and only if there exist z∈Cz\in\mathbb Cz∈C with ∣z∣=1|z|=1∣z∣=1 and an hhh satisfying the stated conditions with U=zG(h)U=zG(h)U=zG(h). Such an injection www cannot exist when n<2n<2n<2.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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