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Appendix A / LP (69): classical-channel one-shot simulation

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QAlgorithms.Papers.Independent.Intakethird100.P65.classical_oneShot_lp

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

prove2quantum

All systems have finite positive dimension and fixed computational bases. Matrix order is Loewner order and logarithms are base two.

Let W(y∣x)W(y|x)W(y∣x) be a finite stochastic channel, with nonempty input and output alphabets, and ε≥0\varepsilon\ge0ε≥0. Embed it as the quantum map X↦∑x,yW(y∣x)Xxx∣y⟩⟨y∣X\mapsto\sum_{x,y}W(y|x)X_{xx}|y\rangle\langle y|X↦∑x,y​W(y∣x)Xxx​∣y⟩⟨y∣. Let tεt_\varepsilontε​ be the infimum of ∑yVy\sum_yV_y∑y​Vy​ over real arrays Yxy,T(y∣x),VyY_{xy},T(y|x),V_yYxy​,T(y∣x),Vy​ satisfying Yxy≥T(y∣x)−W(y∣x)Y_{xy}\ge T(y|x)-W(y|x)Yxy​≥T(y∣x)−W(y∣x), Yxy≥0Y_{xy}\ge0Yxy​≥0, T(y∣x)≥0T(y|x)\ge0T(y∣x)≥0, ∑yT(y∣x)=1\sum_yT(y|x)=1∑y​T(y∣x)=1, T(y∣x)≤VyT(y|x)\le V_yT(y∣x)≤Vy​, and ∑yYxy≤ε\sum_yY_{xy}\le\varepsilon∑y​Yxy​≤ε for every input xxx. Then

SNS,ε(1)(W)=log⁡2⌈tε⌉.S_{\rm NS,\varepsilon}^{(1)}(W)=\log_2\lceil\sqrt{t_\varepsilon}\rceil.SNS,ε(1)​(W)=log2​⌈tε​​⌉.

The linear optimum is attained. The resource is quantum communication even though the target is classical.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P65
Formal statement
noncomputable section

open Filter QAlgorithms

open scoped BigOperators Matrix ComplexConjugate ComplexOrder Topology

namespace QAlgorithms.Papers.Independent.Intakethird100.P65

attribute [local instance] Classical.propDecidable Classical.decEq

open QAlgorithms.Papers.Independent.Dependency50.P09 (transposeBob)

open QAlgorithms.Papers.Independent.Dependency50.P35 (maxRelative)

open QAlgorithms.Papers.Independent.Independent2.P01 (dampingKraus damping)

open QAlgorithms.Papers.Independent.Gap48.P33 (phaseFlipChannel)

open QAlgorithms.Papers.Independent.Information100.P06 (Below)

open QAlgorithms.Papers.Independent.Information100.P34 (choi)

open QAlgorithms.Papers.Independent.Information100.P62 (Stochastic)

open QAlgorithms.Papers.Independent.Information100.P63 (Mat)

open QAlgorithms.Papers.Independent.Information100.P67 (IsSubnormalized purifiedDistance)

open QAlgorithms.Papers.Independent.Information100.P69 (replacer permute)

open QAlgorithms.Papers.Independent.Information100.P71 (diamond channelPower channelRelative)

open QAlgorithms.Papers.Independent.Support50.P39 (quantumMutualInformation)

variable {A B C D R : Type} [Fintype A] [DecidableEq A]
  [Fintype B] [DecidableEq B] [Fintype C] [DecidableEq C]
  [Fintype D] [DecidableEq D] [Fintype R] [DecidableEq R]

variable [Nonempty A] [Nonempty B] [Nonempty C] [Nonempty D] [Nonempty R]

/-- Appendix A, LP (69), PDF p.18: quantum-resource cost for a classical target.
The linear optimum is attained, and every error constraint is per input. -/
theorem classical_oneShot_lp (W : A → B → ℝ) (hW : Stochastic (fun y x => W x y)) (e : ℝ) (he : 0 ≤ e) :
    oneUseSimulationCost .ns (classicalMap W) e = roundedTraceCost (classicalValue W e) ∧
    ∃ Y T : A → B → ℝ, ∃ V : B → ℝ,
      classicalFeasible W e Y T V ∧ (∑ y, V y) = classicalValue W e := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P65

end
Source
Quantum Channel Simulation and the Channel's Smooth Max-Information, arXiv:1807.05354v2, PDF p. 18, Appendix A / LP (69): classical-channel one-shot simulation
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What the Lean code literally says, in plain math · gpt-6.1-sol

For finite types A,BA,BA,B with decidable equality, every function W:A×B→RW:A\times B\to\mathbb RW:A×B→R satisfying W(x,y)≥0W(x,y)\ge0W(x,y)≥0 and ∑yW(x,y)=1\sum_yW(x,y)=1∑y​W(x,y)=1 for every xxx, and every real e≥0e\ge0e≥0, define W(X)=diag⁡y(∑xW(x,y)Xx,x)\mathcal W(X)=\operatorname{diag}_y(\sum_xW(x,y)X_{x,x})W(X)=diagy​(∑x​W(x,y)Xx,x​). Let vev_eve​ be the real infimum of ∑yV(y)\sum_yV(y)∑y​V(y) over real arrays Y,T:A×B→RY,T:A\times B\to\mathbb RY,T:A×B→R and V:B→RV:B\to\mathbb RV:B→R satisfying

T(x,y)−W(x,y)≤Y(x,y),0≤Y(x,y),0≤T(x,y)≤V(y),∑yT(x,y)=1,∑yY(x,y)≤e.T(x,y)-W(x,y)\le Y(x,y),\quad 0\le Y(x,y),\quad 0\le T(x,y)\le V(y),\quad \sum_yT(x,y)=1,\quad \sum_yY(x,y)\le e.T(x,y)−W(x,y)≤Y(x,y),0≤Y(x,y),0≤T(x,y)≤V(y),y∑​T(x,y)=1,y∑​Y(x,y)≤e.

Then cns(W,e)=log⁡2⌈ve⌉c_{\mathrm{ns}}(\mathcal W,e)=\log_2\lceil\sqrt{v_e}\rceilcns​(W,e)=log2​⌈ve​​⌉, and there exist such Y,T,VY,T,VY,T,V with ∑yV(y)=ve\sum_yV(y)=v_e∑y​V(y)=ve​. Here cns(H,e)c_{\mathrm{ns}}(H,e)cns​(H,e) is the real infimum of log⁡2m\log_2 mlog2​m over positive integers mmm for which the infimum of 12∥Wm(P)−H∥⋄\tfrac12\|\mathcal W_m(P)-H\|_\diamond21​∥Wm​(P)−H∥⋄​ is at most eee, with the latter infimum over channels P:Mat⁡(A×{0,…,m−1})→Mat⁡({0,…,m−1}×B)P:\operatorname{Mat}(A\times\{0,\ldots,m-1\})\to\operatorname{Mat}(\{0,\ldots,m-1\}\times B)P:Mat(A×{0,…,m−1})→Mat({0,…,m−1}×B) whose output marginals each depend only on the corresponding input marginal; Wm(P)(X)b,d=∑a,c<mP(X⊗∣a⟩⟨c∣)(a,b),(c,d)\mathcal W_m(P)(X)_{b,d}=\sum_{a,c<m}P(X\otimes|a\rangle\langle c|)_{(a,b),(c,d)}Wm​(P)(X)b,d​=∑a,c<m​P(X⊗∣a⟩⟨c∣)(a,b),(c,d)​. A channel is a finite Kraus map with ∑jKj†Kj=I\sum_jK_j^\dagger K_j=I∑j​Kj†​Kj​=I, and ∥F∥⋄=sup⁡∥X∥1≤1∥(idA⊗F)(X)∥1\|F\|_\diamond=\sup_{\|X\|_1\le1}\|(\mathrm{id}_A\otimes F)(X)\|_1∥F∥⋄​=sup∥X∥1​≤1​∥(idA​⊗F)(X)∥1​, over arbitrary matrices on A×AA\times AA×A, where ∥X∥1=Re⁡tr⁡X†X\|X\|_1=\operatorname{Re}\operatorname{tr}\sqrt{X^\dagger X}∥X∥1​=RetrX†X​. The ceiling is the natural-number ceiling. There is no upper bound on eee; e=0e=0e=0 is included. Empty finite types are not explicitly excluded: if A≠∅A\ne\varnothingA=∅ and B=∅B=\varnothingB=∅, the stochasticity hypothesis is impossible. Real infima use value 000 when empty or unbounded below, x=0\sqrt{x}=0x​=0 for x<0x<0x<0, and log⁡20=0\log_2 0=0log2​0=0.

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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