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Proposition 4: continuous SWAP coupling approximates density-matrix evolution

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QAlgorithms.Papers.Independent.Intakethird100.P67.proposition4_continuous_swap

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

prove2quantum

Prepare n≥1n\ge1n≥1 independent reference registers in the same unit vector ϕ\phiϕ, a system density operator ρ\rhoρ, a real coupling JJJ, and time t≥0t\ge0t≥0. Let H=J∑j=1nSWAP⁡S,jH=J\sum_{j=1}^n\operatorname{SWAP}_{S,j}H=J∑j=1n​SWAPS,j​, Heff=J(n+1)∣ϕ⟩⟨ϕ∣H_{\rm eff}=J(n+1)|\phi\rangle\langle\phi|Heff​=J(n+1)∣ϕ⟩⟨ϕ∣, and let ρ(t)\rho(t)ρ(t) be the actual system partial trace of the joint evolution. Then

F(ρ(t),e−itHeffρeitHeff)≥n−1n+1,12∥ρ(t)−e−itHeffρeitHeff∥1≤6n.F(\rho(t),e^{-itH_{\rm eff}}\rho e^{itH_{\rm eff}})\ge\frac{n-1}{n+1},\qquad\tfrac12\|\rho(t)-e^{-itH_{\rm eff}}\rho e^{itH_{\rm eff}}\|_1\le\frac6n.F(ρ(t),e−itHeff​ρeitHeff​)≥n+1n−1​,21​∥ρ(t)−e−itHeff​ρeitHeff​∥1​≤n6​.

For every normalized pure system input ψ\psiψ, the absolute overlap of e−itH(∣ψ⟩∣ϕ⟩⊗n)e^{-itH}(|\psi\rangle|\phi\rangle^{\otimes n})e−itH(∣ψ⟩∣ϕ⟩⊗n) with (e−itHeff∣ψ⟩)∣ϕ⟩⊗n(e^{-itH_{\rm eff}}|\psi\rangle)|\phi\rangle^{\otimes n}(e−itHeff​∣ψ⟩)∣ϕ⟩⊗n is at least (n−1)/(n+1)(n-1)/(n+1)(n−1)/(n+1). These joint and reduced bounds refer to the same physical evolution.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P67
Formal statement
noncomputable section

open scoped ComplexConjugate Matrix Matrix.Norms.L2Operator

attribute [local instance] Classical.propDecidable

open MeasureTheory Filter

namespace QAlgorithms.Papers.Independent.Intakethird100.P67

variable {I J K L A : Type*} [Fintype I] [DecidableEq I]
  [Fintype J] [DecidableEq J] [Fintype K] [DecidableEq K]
  [Fintype L] [DecidableEq L] [Fintype A] [DecidableEq A]

/-- PDF p.24, Proposition 4, E4–E6: both reduced-state estimates and the absolute
joint overlap. Real subtraction prevents truncation at n=1; n=0 is excluded. -/
theorem proposition4_continuous_swap (phi : EuclideanSpace ℂ I) (hphi : IsState phi)
    (n : ℕ) (hn : 1 ≤ n) (coupling t : ℝ) (ht : 0 ≤ t) :
    (∀ rho : Matrix I I ℂ, IsDensityMatrix rho →
      let actual := traceRight (swapJoint phi n coupling t rho)
      let target := densityConjugation (positivePhaseEvolution (effectiveHamiltonian phi n coupling) (-t)) rho
      ((n : ℝ) - 1) / (n + 1) ≤ rootFidelity actual target ∧ traceDistance actual target ≤ 6 / n) ∧
    (∀ psi : EuclideanSpace ℂ I, IsState psi → ((n : ℝ) - 1) / (n + 1) ≤
      ‖inner ℂ (tensorVec (act (positivePhaseEvolution (effectiveHamiltonian phi n coupling) (-t)) psi)
        (referenceVector phi n)) (act (positivePhaseEvolution (swapHamiltonian n coupling) (-t))
          (tensorVec psi (referenceVector phi n)))‖) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P67

end
Source
Universal Quantum Emulator, arXiv:1606.02734v2, PDF p. 24, Proposition 4: continuous SWAP coupling approximates density-matrix evolution
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let III be a finite index type with decidable equality, let ϕ∈CI\phi\in\mathbb C^Iϕ∈CI have norm 111, let n≥1n\ge1n≥1 be a natural number, let c∈Rc\in\mathbb Rc∈R be arbitrary, and let t≥0t\ge0t≥0. Put P=ϕϕ†P=\phi\phi^\daggerP=ϕϕ†, Φn=ϕ⊗n\Phi_n=\phi^{\otimes n}Φn​=ϕ⊗n, Heff=c(n+1)PH_{\mathrm{eff}}=c(n+1)PHeff​=c(n+1)P, and Hswap=c∑j=0n−1SjH_{\mathrm{swap}}=c\sum_{j=0}^{n-1}S_jHswap​=c∑j=0n−1​Sj​, where SjS_jSj​ swaps the system register with reference register jjj: on basis labels it sends (i,(xℓ)ℓ)(i,(x_\ell)_\ell)(i,(xℓ​)ℓ​) to (xj,(xℓ)ℓ≠j,i at j)(x_j,(x_\ell)_{\ell\ne j},i\text{ at }j)(xj​,(xℓ​)ℓ=j​,i at j). For every positive semidefinite matrix ρ\rhoρ of trace 111, define

A=Tr⁡ref ⁣[e−itHswap(ρ⊗ΦnΦn†)eitHswap],B=e−itHeffρeitHeff.A=\operatorname{Tr}_{\mathrm{ref}}\!\left[ e^{-itH_{\mathrm{swap}}}(\rho\otimes\Phi_n\Phi_n^\dagger)e^{itH_{\mathrm{swap}}} \right], \qquad B=e^{-itH_{\mathrm{eff}}}\rho e^{itH_{\mathrm{eff}}}.A=Trref​[e−itHswap​(ρ⊗Φn​Φn†​)eitHswap​],B=e−itHeff​ρeitHeff​.

Then

n−1n+1≤Re⁡tr⁡A BA,12Re⁡tr⁡(A−B)†(A−B)≤6n,\frac{n-1}{n+1} \le\operatorname{Re}\operatorname{tr}\sqrt{\sqrt A\,B\sqrt A}, \qquad \tfrac12\operatorname{Re}\operatorname{tr}\sqrt{(A-B)^\dagger(A-B)} \le\frac6n,n+1n−1​≤RetrA​BA​​,21​Retr(A−B)†(A−B)​≤n6​,

with square roots defined by functional calculus. In addition, for every norm-111 vector ψ∈CI\psi\in\mathbb C^Iψ∈CI,

n−1n+1≤∣⟨(e−itHeffψ)⊗Φn, e−itHswap(ψ⊗Φn)⟩∣.\frac{n-1}{n+1} \le \left| \left\langle (e^{-itH_{\mathrm{eff}}}\psi)\otimes\Phi_n,\, e^{-itH_{\mathrm{swap}}}(\psi\otimes\Phi_n) \right\rangle \right|.n+1n−1​≤​⟨(e−itHeff​ψ)⊗Φn​,e−itHswap​(ψ⊗Φn​)⟩​.

The case n=1n=1n=1 is included; no sign or magnitude restriction is imposed on ccc, and there is no upper bound on ttt.

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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