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Lemma 8: corrected white-noise conversion criterion

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QAlgorithms.Papers.Independent.Intakethird100.P19.whiteNoise_conversion

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

prove2quantum

All Hilbert spaces are finite-dimensional complex spaces with fixed product bases and positive local dimensions. States are positive semidefinite operators of trace one; pure kets have norm one. Let k,d≥2k,d\ge2k,d≥2, with pure states ψ\psiψ on k×kk\times kk×k and φ\varphiφ on d×dd\times dd×d, and decreasing squared Schmidt coefficients λi,μi\lambda_i,\mu_iλi​,μi​. Define

Λ(X)=Tr⁡(ψX)φ+Tr⁡((Ik2−ψ)X)Id2d2.\Lambda(X)=\operatorname{Tr}(\psi X)\varphi+\operatorname{Tr}((I_{k^2}-\psi)X)\frac{I_{d^2}}{d^2}.Λ(X)=Tr(ψX)φ+Tr((Ik2​−ψ)X)d2Id2​​.

This is a channel and is non-entangling if (1+d2μ1μ2)λ1≤1(1+d^2\sqrt{\mu_1\mu_2})\lambda_1\le1(1+d2μ1​μ2​​)λ1​≤1. Under this condition it is also dually non-entangling if

(d2μ1−1)λ1λ2≤1.(d^2\mu_1-1)\sqrt{\lambda_1\lambda_2}\le1.(d2μ1​−1)λ1​λ2​​≤1.

Dually non-entangling means that both the channel and its trace dual preserve separable positive operators.

The cross-multiplied inequalities retain product-state cases.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P19
Formal statement
noncomputable section

open QAlgorithms QAlgorithms.Entanglement Filter

open scoped Matrix ComplexOrder ComplexConjugate ENNReal

attribute [local instance] Classical.propDecidable Classical.decEq

namespace QAlgorithms.Papers.Independent.Intakethird100.P19

open QAlgorithms.Papers.Independent.Information100.P21 (Op FiniteLOCC)

open QAlgorithms.Papers.Independent.Information100.P19 (Bip)

open QAlgorithms.Papers.Independent.Information100.P69 (CP)

open QAlgorithms.Papers.Independent.Information100.P71 (supportPower SupportIncluded)

open QAlgorithms.Papers.Independent.Dependency50.P19 (epr)

/-- Lemma 8, PDF pp.11-12, corrected from its proof: printed Eq.(8)
omits 1+ in the denominator. Use (1+d^2 sqrt(mu_1 mu_2))*lambda_1<=1.
Eq.(9) is cross-multiplied to include zero second Schmidt coefficients.
The printed Bell-to-Bell case violates PPT preservation of separable inputs. -/
theorem whiteNoise_conversion {k d : ℕ} (hk : 2 ≤ k) (hd : 2 ≤ d)
    (psi : UnitBipartiteKet k k) (phi : UnitBipartiteKet d d)
    (hfirst : (1 + (d : ℝ) ^ 2 * Real.sqrt (schmidtAt phi.ket 0 * schmidtAt phi.ket 1)) *
      schmidtAt psi.ket 0 ≤ 1) :
    let L := binaryMeasurePrepare psi.rho phi.rho (((d : ℂ) ^ 2)⁻¹ • (1 : Bip d d))
    IsChannel L ∧ NE L ∧
      (((d : ℝ) ^ 2 * schmidtAt phi.ket 0 - 1) *
        Real.sqrt (schmidtAt psi.ket 0 * schmidtAt psi.ket 1) ≤ 1 → DNE L) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P19

end
Source
Entanglement manipulation and distillability beyond LOCC, arXiv:1711.03835v2, PDF p. 11, Lemma 8
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What the Lean code literally says, in plain math · gpt-6.1-sol

For all natural numbers k,d≥2k,d\ge2k,d≥2 and unit vectors ψ∈Ck⊗Ck\psi\in\mathbb C^k\otimes\mathbb C^kψ∈Ck⊗Ck and ϕ∈Cd⊗Cd\phi\in\mathbb C^d\otimes\mathbb C^dϕ∈Cd⊗Cd, let Pψ=∣ψ⟩⟨ψ∣P_\psi=|\psi\rangle\langle\psi|Pψ​=∣ψ⟩⟨ψ∣ and Pϕ=∣ϕ⟩⟨ϕ∣P_\phi=|\phi\rangle\langle\phi|Pϕ​=∣ϕ⟩⟨ϕ∣. For either vector vvv, let λ0(v)\lambda_0(v)λ0​(v) and λ1(v)\lambda_1(v)λ1​(v) be the largest and second-largest eigenvalues, counting multiplicities, of its first marginal (∑jvijvi′j‾)i,i′(\sum_jv_{ij}\overline{v_{i'j}})_{i,i'}(∑j​vij​vi′j​​)i,i′​; these include zero eigenvalues. If (1+d2λ0(ϕ)λ1(ϕ))λ0(ψ)≤1(1+d^2\sqrt{\lambda_0(\phi)\lambda_1(\phi)})\lambda_0(\psi)\le1(1+d2λ0​(ϕ)λ1​(ϕ)​)λ0​(ψ)≤1, define the map LLL on every input operator by L(X)=Tr⁡(PψX)Pϕ+Tr⁡((I−Pψ)X)Id2/d2L(X)=\operatorname{Tr}(P_\psi X)P_\phi+\operatorname{Tr}((I-P_\psi)X)I_{d^2}/d^2L(X)=Tr(Pψ​X)Pϕ​+Tr((I−Pψ​)X)Id2​/d2. Then LLL is a channel and is non-entangling. Moreover, if (d2λ0(ϕ)−1)λ0(ψ)λ1(ψ)≤1(d^2\lambda_0(\phi)-1)\sqrt{\lambda_0(\psi)\lambda_1(\psi)}\le1(d2λ0​(ϕ)−1)λ0​(ψ)λ1​(ψ)​≤1, then both LLL and its trace-bilinear dual are non-entangling. Here a channel has a finite Kraus representation L(X)=∑jEjXEj†L(X)=\sum_jE_jXE_j^\daggerL(X)=∑j​Ej​XEj†​ with ∑jEj†Ej=I\sum_jE_j^\dagger E_j=I∑j​Ej†​Ej​=I; a non-entangling map has a finite Kraus representation, without a normalization requirement, and preserves the cone of finite nonnegative sums of tensor products of positive semidefinite trace-one matrices, including the empty sum. The trace-bilinear dual is defined entrywise by (L∨(Y))ij=Tr⁡(L(Eji)Y)(L^\vee(Y))_{ij}=\operatorname{Tr}(L(E_{ji})Y)(L∨(Y))ij​=Tr(L(Eji​)Y), where EjiE_{ji}Eji​ is the input matrix unit.

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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