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Proposition 13: nonnegativity and exact reference equality conditions

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QAlgorithms.Papers.Independent.Intakethird100.P52.renyi_nonnegative_iff_reference

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

prove2quantum

All Hilbert spaces below are finite dimensional and nonzero over C\mathbb CC. A density operator is positive semidefinite with trace one. Every spectral power is zero on the kernel, including zero and negative powers. Information quantities use base-two logarithms, with log⁡20=−∞\log_2 0=-\inftylog2​0=−∞; the operator logarithms in exponential formulas are natural logarithms.

Let ρ\rhoρ be a density operator on HHH, let σ≥0\sigma\ge0σ≥0 be an operator on HHH without a trace constraint, and let N:B(H)→B(K)\mathcal N:\mathcal B(H)\to\mathcal B(K)N:B(H)→B(K) be CPTP. Its adjoint N†\mathcal N^\daggerN† is the Hilbert–Schmidt adjoint. Write

Ka=σ(1−a)/2N† ⁣(N(σ)(a−1)/2N(ρ)1−aN(σ)(a−1)/2)σ(1−a)/2,La=σ(1−a)/(2a)N† ⁣(N(σ)(a−1)/(2a)N(ρ)(1−a)/aN(σ)(a−1)/(2a))σ(1−a)/(2a),Ra=Ka1/(1−a),Sa=Laa/(1−a),Δa=log⁡2Tr⁡(ρaKa)a−1,Δ~a=log⁡2Tr⁡[(ρ1/2Laρ1/2)a]a−1.\begin{aligned} K_a&=\sigma^{(1-a)/2}\mathcal N^\dagger\!\left(\mathcal N(\sigma)^{(a-1)/2}\mathcal N(\rho)^{1-a}\mathcal N(\sigma)^{(a-1)/2}\right)\sigma^{(1-a)/2},\\ L_a&=\sigma^{(1-a)/(2a)}\mathcal N^\dagger\!\left(\mathcal N(\sigma)^{(a-1)/(2a)}\mathcal N(\rho)^{(1-a)/a}\mathcal N(\sigma)^{(a-1)/(2a)}\right)\sigma^{(1-a)/(2a)},\\ R_a&=K_a^{1/(1-a)},\qquad S_a=L_a^{a/(1-a)},\\ \Delta_a&=\frac{\log_2\operatorname{Tr}(\rho^aK_a)}{a-1},\qquad \widetilde\Delta_a=\frac{\log_2\operatorname{Tr}[(\rho^{1/2}L_a\rho^{1/2})^a]}{a-1}. \end{aligned}Ka​La​Ra​Δa​​=σ(1−a)/2N†(N(σ)(a−1)/2N(ρ)1−aN(σ)(a−1)/2)σ(1−a)/2,=σ(1−a)/(2a)N†(N(σ)(a−1)/(2a)N(ρ)(1−a)/aN(σ)(a−1)/(2a))σ(1−a)/(2a),=Ka1/(1−a)​,Sa​=Laa/(1−a)​,=a−1log2​Tr(ρaKa​)​,Δa​=a−1log2​Tr[(ρ1/2La​ρ1/2)a]​.​

For the indicated ranges,

0<a<1:Δa≥0,(Δa=0  ⟺  ρ=Ra),1/2<a<1:Δ~a≥0,(Δ~a=0  ⟺  ρ=Sa).\begin{aligned} 0<a<1 &: \quad\Delta_a\ge0,\qquad (\Delta_a=0\iff\rho=R_a),\\ 1/2<a<1 &: \quad\widetilde\Delta_a\ge0,\qquad (\widetilde\Delta_a=0\iff\rho=S_a). \end{aligned}0<a<11/2<a<1​:Δa​≥0,(Δa​=0⟺ρ=Ra​),:Δa​≥0,(Δa​=0⟺ρ=Sa​).​

If ρ,σ,N(ρ),N(σ)>0\rho,\sigma,\mathcal N(\rho),\mathcal N(\sigma)>0ρ,σ,N(ρ),N(σ)>0, the first pair of conclusions also holds for 1<a<21<a<21<a<2, and the second for every a>1a>1a>1.

Nonnegativity and exact equality to the computed reference are both parts of the result.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P52
Formal statement
noncomputable section

open scoped Matrix ComplexOrder

namespace QAlgorithms.Papers.Independent.Intakethird100.P52

attribute [local instance] Classical.propDecidable Classical.decEq

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

open QAlgorithms.Papers.Independent.Dependency50.P21 (channelAdjoint petz marginalAB)

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

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

open QAlgorithms.Papers.Independent.Renew46.P35 (HasMarkovBlocks)

/-- Proposition 13, PDF p.14, equations (3.56)–(3.59). Each equality condition
is a conclusion. No support containment or strictness is added below one. -/
theorem renyi_nonnegative_iff_reference {H K : Type} [Fintype H] [Fintype K]
    [DecidableEq H] [DecidableEq K] [Nonempty H] [Nonempty K]
    (rho sigma : Mat H) (hrho : IsDensityMatrix rho)
    (hsigma : sigma.PosSemidef) (N : Superop H K) (hN : IsChannel N) :
    (∀ a : ℝ, 0 < a ∧ a < 1 →
      0 ≤ renyiDifference a rho sigma N ∧
      (renyiDifference a rho sigma N = 0 ↔ rho = renyiReference a rho sigma N)) ∧
    (∀ a : ℝ, 1 / 2 < a ∧ a < 1 →
      0 ≤ deltaTilde a rho sigma N ∧
      (deltaTilde a rho sigma N = 0 ↔ rho = sandwichedReference a rho sigma N)) ∧
    ((rho.PosDef ∧ sigma.PosDef ∧ (N rho).PosDef ∧ (N sigma).PosDef) →
      (∀ a : ℝ, 1 < a ∧ a < 2 →
        0 ≤ renyiDifference a rho sigma N ∧
        (renyiDifference a rho sigma N = 0 ↔ rho = renyiReference a rho sigma N)) ∧
      (∀ a : ℝ, 1 < a →
        0 ≤ deltaTilde a rho sigma N ∧
        (deltaTilde a rho sigma N = 0 ↔ rho = sandwichedReference a rho sigma N))) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P52

end
Source
Quantum Markov chains, sufficiency of quantum channels, and Renyi information measures, arXiv:1501.05636v4, PDF p. 14, Proposition 13: nonnegativity and exact reference equality conditions
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let H,KH,KH,K be finite nonempty types with decidable equality, let ρ\rhoρ be a positive semidefinite complex matrix on HHH with trace 111, let σ\sigmaσ be any positive semidefinite complex matrix on HHH, and let N(X)=∑jEjXEj†N(X)=\sum_jE_jXE_j^\daggerN(X)=∑j​Ej​XEj†​ be a channel with a finite Kraus family satisfying ∑jEj†Ej=IH\sum_jE_j^\dagger E_j=I_H∑j​Ej†​Ej​=IH​. Define (N†Z)ij=∑k,lN(Eij)kl‾Zkl(N^\dagger Z)_{ij}=\sum_{k,l}\overline{N(E_{ij})_{kl}}Z_{kl}(N†Z)ij​=∑k,l​N(Eij​)kl​​Zkl​, and let St(X)S_t(X)St​(X) be continuous functional calculus for the function zero at zero and xtx^txt otherwise. Put

Ka=S(1−a)/2(σ)N† ⁣(S(a−1)/2(Nσ)S1−a(Nρ)S(a−1)/2(Nσ))S(1−a)/2(σ),K~a=S(1−a)/(2a)(σ)N† ⁣(S(a−1)/(2a)(Nσ)S(1−a)/a(Nρ)S(a−1)/(2a)(Nσ))S(1−a)/(2a)(σ),Ra=S1/(1−a)(Ka),R~a=Sa/(1−a)(K~a),Da=ℓ2(Re⁡Tr⁡(Sa(ρ)Ka))a−1,D~a=ℓ2(Re⁡Tr⁡Sa(S1/2(ρ)K~aS1/2(ρ)))a−1,\begin{aligned} K_a&=S_{(1-a)/2}(\sigma) N^\dagger\!\left(S_{(a-1)/2}(N\sigma)S_{1-a}(N\rho)S_{(a-1)/2}(N\sigma)\right) S_{(1-a)/2}(\sigma),\\ \widetilde K_a&=S_{(1-a)/(2a)}(\sigma) N^\dagger\!\left(S_{(a-1)/(2a)}(N\sigma)S_{(1-a)/a}(N\rho)S_{(a-1)/(2a)}(N\sigma)\right) S_{(1-a)/(2a)}(\sigma),\\ R_a&=S_{1/(1-a)}(K_a),\qquad \widetilde R_a=S_{a/(1-a)}(\widetilde K_a),\\ D_a&=\frac{\ell_2(\operatorname{Re}\operatorname{Tr}(S_a(\rho)K_a))}{a-1},\\ \widetilde D_a&=\frac{\ell_2(\operatorname{Re}\operatorname{Tr}S_a(S_{1/2}(\rho)\widetilde K_aS_{1/2}(\rho)))}{a-1}, \end{aligned}Ka​Ka​Ra​Da​Da​​=S(1−a)/2​(σ)N†(S(a−1)/2​(Nσ)S1−a​(Nρ)S(a−1)/2​(Nσ))S(1−a)/2​(σ),=S(1−a)/(2a)​(σ)N†(S(a−1)/(2a)​(Nσ)S(1−a)/a​(Nρ)S(a−1)/(2a)​(Nσ))S(1−a)/(2a)​(σ),=S1/(1−a)​(Ka​),Ra​=Sa/(1−a)​(Ka​),=a−1ℓ2​(ReTr(Sa​(ρ)Ka​))​,=a−1ℓ2​(ReTrSa​(S1/2​(ρ)Ka​S1/2​(ρ)))​,​

where ℓ2(x)=log⁡2x\ell_2(x)=\log_2xℓ2​(x)=log2​x for x>0x>0x>0 and −∞-\infty−∞ otherwise, and Da,D~aD_a,\widetilde D_aDa​,Da​ are extended real. For every 0<a<10<a<10<a<1, the assertion is 0≤Da0\le D_a0≤Da​ and Da=0D_a=0Da​=0 if and only if ρ=Ra\rho=R_aρ=Ra​; for every 1/2<a<11/2<a<11/2<a<1, it is 0≤D~a0\le\widetilde D_a0≤Da​ and D~a=0\widetilde D_a=0Da​=0 if and only if ρ=R~a\rho=\widetilde R_aρ=Ra​. If all four matrices ρ,σ,Nρ,Nσ\rho,\sigma,N\rho,N\sigmaρ,σ,Nρ,Nσ are positive definite, the first pair of assertions also holds for every 1<a<21<a<21<a<2, and the second for every a>1a>1a>1. No trace normalization of σ\sigmaσ or support-inclusion hypothesis is imposed; the first two parameter ranges include singular matrices and σ=0\sigma=0σ=0, using the stated zero-value convention for powers and extended logarithms.

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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