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Amplitude-damping complement has commuting basis outputs

Proved
QAlgorithms.Papers.Independent.Intakethird100.P10.amplitudeDamping_classical_environment

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

prove2quantum

Let 0≤γ≤10\le\gamma\le10≤γ≤1 be the original amplitude-damping probability. Its printed complementary map is the linear map with diagonal entries ρ00+(1−γ)ρ11\rho_{00}+(1-\gamma)\rho_{11}ρ00​+(1−γ)ρ11​ and γρ11\gamma\rho_{11}γρ11​, and off-diagonal entries γρ01\sqrt\gamma\rho_{01}γ​ρ01​ and γρ10\sqrt\gamma\rho_{10}γ​ρ10​. On the computational-basis states,

W∗(∣0⟩⟨0∣)=∣0⟩⟨0∣,W∗(∣1⟩⟨1∣)=(1−γ)∣0⟩⟨0∣+γ∣1⟩⟨1∣.W^*(|0\rangle\langle0|)=|0\rangle\langle0|,\qquad W^*(|1\rangle\langle1|)=(1-\gamma)|0\rangle\langle0|+\gamma|1\rangle\langle1|.W∗(∣0⟩⟨0∣)=∣0⟩⟨0∣,W∗(∣1⟩⟨1∣)=(1−γ)∣0⟩⟨0∣+γ∣1⟩⟨1∣.

The two outputs commute. This supplies the classical-environment criterion for the specified basis; no all-parameter degradability claim is made.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P10
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P10

open scoped BigOperators Matrix ComplexConjugate

open Filter

-- Accepted definitions, without paper-local aliases.

open QAlgorithms.Papers.Independent.Information100.P58 (basisDensity)

open QAlgorithms.Papers.Independent.Information100.P67 (squaredFidelity)

open QAlgorithms.Papers.Independent.Claimed50.P48 (indexedKrausDilation)

/-- PDF pp.10–11, Appendix B: the two amplitude-damping complement outputs,
and their commutation, for every damping parameter in [0,1]. No degradability claim. -/
theorem amplitudeDamping_classical_environment (gamma : ℝ) (hlo : 0 ≤ gamma) (hhi : gamma ≤ 1) :
    amplitudeComplement gamma (basisDensity false) = basisDensity false ∧
    amplitudeComplement gamma (basisDensity true) =
      ((1 - gamma : ℝ) : ℂ) • basisDensity false + (gamma : ℂ) • basisDensity true ∧
    Commute (amplitudeComplement gamma (basisDensity false))
      (amplitudeComplement gamma (basisDensity true)) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P10

end
Source
Polar codes for degradable quantum channels, arXiv:1109.5346v3, PDF p. 11, Appendix B, unnumbered amplitude-damping classical-environment example
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every real γ\gammaγ satisfying 0≤γ≤10\le\gamma\le10≤γ≤1, let E0=diag⁡(1,0)E_0=\operatorname{diag}(1,0)E0​=diag(1,0), E1=diag⁡(0,1)E_1=\operatorname{diag}(0,1)E1​=diag(0,1), and define

Aγ(ρ)=(ρ00+(1−γ)ρ11γρ01γρ10γρ11).\mathcal A_\gamma(\rho)= \begin{pmatrix} \rho_{00}+(1-\gamma)\rho_{11}&\sqrt{\gamma}\rho_{01}\\ \sqrt{\gamma}\rho_{10}&\gamma\rho_{11} \end{pmatrix}.Aγ​(ρ)=(ρ00​+(1−γ)ρ11​γ​ρ10​​γ​ρ01​γρ11​​).

Then Aγ(E0)=E0\mathcal A_\gamma(E_0)=E_0Aγ​(E0​)=E0​, Aγ(E1)=(1−γ)E0+γE1\mathcal A_\gamma(E_1)=(1-\gamma)E_0+\gamma E_1Aγ​(E1​)=(1−γ)E0​+γE1​, and these two output matrices commute, meaning their products in the two orders are equal. Both endpoints γ=0\gamma=0γ=0 and γ=1\gamma=1γ=1 are included.

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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