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Nearest-neighbour matchgates admit strong classical simulation

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QAlgorithms.Papers.Independent.Intakethird100.P77.nearestNeighbour_strongSimulation

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

prove2quantum

Let a uniformly described circuit family consist of two-qubit parity-block gates G(A,B)G(A,B)G(A,B), where A,BA,BA,B are unitary and det⁡A=det⁡B\det A=\det BdetA=detB, placed only on adjacent wires of a fixed path. Let the input on each wire be an independently normalized one-qubit pure state. Circuit structure, gate entries, and input amplitudes have polynomial-time finite bit descriptions to requested precision. For every existing output wire kkk and outcome b∈{0,1}b\in\{0,1\}b∈{0,1}, a single deterministic classical polynomial-time machine computes a dyadic qqq such that

∣q−pb∣≤2−m,pb=1+(−1)b⟨Zk⟩out2.|q-p_b|\le 2^{-m},\qquad p_b=\frac{1+(-1)^b\langle Z_k\rangle_{\rm out}}2.∣q−pb​∣≤2−m,pb​=21+(−1)b⟨Zk​⟩out​​.

The machine is fixed before the instance description, wire, outcome and requested precision mmm. Its time includes the description cost and precision. This is strong simulation of a single final measurement for arbitrary product inputs, including inputs without definite fermionic parity.

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 p.2 Theorem 1, with the precision convention of p.3. Arbitrary
normalized product inputs are allowed. The common phase of an equal-determinant
matchgate is retained; the local Gaussian identification on p.11 requires the
phase correction recorded in HARD.md. -/
theorem nearestNeighbour_strongSimulation (F : ParityFamily)
    (I : ProductInputs F.width) (hF : F.Effective)
    (hI : EffectiveNumbers I.data)
    (hmatch : ∀ s g, g ∈ F.gates s → g.Allowable)
    (hpath : ∀ s, RangeBound 1 (F.gates s)) :
    StrongSimulation F.width (fun s k b =>
      singleWireProbability (parityCircuit (F.gates s)).unitary (prodState (I.factor s)) k b) ∧
    (∀ s (k : Fin (F.width s)) b,
      singleWireProbability (parityCircuit (F.gates s)).unitary (prodState (I.factor s)) k b =
        (1 + (if b then -1 else 1) *
          (outputExpectation (parityCircuit (F.gates s)).unitary
            (prodState (I.factor s)) (zOperator k)).re) / 2) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P77

end
Source
Matchgates and classical simulation of quantum circuits, arXiv:0804.4050v2, PDF p. 2, Theorem 1 / abstract seed: nearest-neighbour matchgate strong simulation
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let FFF assign to every finite Boolean string sss a natural width w(s)w(s)w(s) and a finite ordered list of applications, each containing unitary 2×22\times22×2 complex matrices Ag,BgA_g,B_gAg​,Bg​ and two distinct ordered wire indices. Let III assign a unit-norm two-component complex vector ϕs,i\phi_{s,i}ϕs,i​ to each wire i<w(s)i<w(s)i<w(s). Assume that every application satisfies det⁡Ag=det⁡Bg\det A_g=\det B_gdetAg​=detBg​, and that the absolute difference between its two wire indices is at most 111. Assume also the following effectiveness conditions. Write u(k)u(k)u(k) for kkk true bits and TTT for the encoding that concatenates, for each constituent string xxx, the prefix u(∣x∣)u(|x|)u(∣x∣), a false bit, and xxx. The structural string T([u(w(s)),u(L),T([u(i1),u(j1)]),…,T([u(iL),u(jL)])])T([u(w(s)),u(L),T([u(i_1),u(j_1)]),\ldots,T([u(i_L),u(j_L)])])T([u(w(s)),u(L),T([u(i1​),u(j1​)]),…,T([u(iL​),u(jL​)])]), where LLL is the application count, must be computable exactly in polynomial time. For each of the two complex data lists—first, the entries 00,01,10,1100,01,10,1100,01,10,11 of AgA_gAg​ followed by those of BgB_gBg​, application by application; second, the false and true components of ϕs,i\phi_{s,i}ϕs,i​, wire by wire—there must be a polynomial-time string function which, on T([s,u(j),u(m),[b]])T([s,u(j),u(m),[b]])T([s,u(j),u(m),[b]]), approximates the indicated entry’s real component when bbb is false or imaginary component when bbb is true, to absolute error at most 2−m2^{-m}2−m, for every valid index jjj and natural precision mmm. Here an output string is interpreted as a signed binary integer divided by 2m2^m2m, with its first bit indicating a negative sign when true and its remaining bits giving the binary magnitude; missing bits contribute zero. Define the input vector by Ψs(x)=∏i<w(s)ϕs,i(xi)\Psi_s(x)=\prod_{i<w(s)}\phi_{s,i}(x_i)Ψs​(x)=∏i<w(s)​ϕs,i​(xi​). An application acts on its ordered pair of wires by the matrix whose x,yx,yx,y entry is zero if x0xorx1≠y0xory1x_0\mathbin{\mathrm{xor}}x_1\ne y_0\mathbin{\mathrm{xor}}y_1x0​xorx1​=y0​xory1​, and otherwise is (Bg)x0y0(B_g)_{x_0y_0}(Bg​)x0​y0​​ for odd parity and (Ag)x0y0(A_g)_{x_0y_0}(Ag​)x0​y0​​ for even parity; embedding it on all wires gives zero between strings that differ outside the selected pair. Let UsU_sUs​ be the product of these embedded matrices in reverse list order, so the first listed application acts first. Then there exists a polynomial-time computable string function fff such that, for every sss, natural mmm, wire k<w(s)k<w(s)k<w(s), and Boolean bbb, the signed dyadic value of f(T([s,u(m),u(k),[b]]))f(T([s,u(m),u(k),[b]]))f(T([s,u(m),u(k),[b]])) approximates

ps,k,b:=∑x∈{0,1}w(s)xk=b∣(UsΨs)x∣2p_{s,k,b}:=\sum_{\substack{x\in\{0,1\}^{w(s)}\\x_k=b}}|(U_s\Psi_s)_x|^2ps,k,b​:=x∈{0,1}w(s)xk​=b​∑​∣(Us​Ψs​)x​∣2

to absolute error at most 2−m2^{-m}2−m. Moreover, for every such s,k,bs,k,bs,k,b,

ps,k,b=1+ϵb Re⁡⟨UsΨs,ZkUsΨs⟩2,ϵfalse=1,ϵtrue=−1,p_{s,k,b} =\frac{1+\epsilon_b\,\operatorname{Re}\langle U_s\Psi_s,Z_kU_s\Psi_s\rangle}{2}, \qquad \epsilon_{\mathrm{false}}=1,\quad\epsilon_{\mathrm{true}}=-1,ps,k,b​=21+ϵb​Re⟨Us​Ψs​,Zk​Us​Ψs​⟩​,ϵfalse​=1,ϵtrue​=−1,

where ZkZ_kZk​ is diagonal with entry 111 on strings whose kkk-th bit is false and −1-1−1 on strings whose kkk-th bit is true, and the inner product conjugates its first argument. Empty application lists give the identity. Width zero is allowed, with an empty application list and an empty product defining Ψs=1\Psi_s=1Ψs​=1; all conclusions requiring a wire index are then vacuous.

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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