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Explicit alpha-family estimates and the strict irreversibility chain

Open
QAlgorithms.Papers.Independent.Intakethird100.P90.alpha_family_irreversibility

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

prove2quantum

All systems are finite-dimensional complex Hilbert spaces with fixed orthonormal product bases and positive local dimensions. A state is a positive semidefinite operator of trace one. All logarithms are base two and all operational rates are measured in standard Bell pairs (ebits) per input copy, with deterministic operations and error tending to zero. Write ED,ECE_D,E_CED​,EC​ for distillable entanglement and entanglement cost under completely PPT-preserving CPTP operations; an explicit LOCC subscript denotes unrestricted two-way local operations and classical communication.

Let 21/50≤α≤1/221/50\le\alpha\le1/221/50≤α≤1/2, ψ1=α∣01⟩−1−α∣10⟩\psi_1=\sqrt\alpha|01\rangle-\sqrt{1-\alpha}|10\rangleψ1​=α​∣01⟩−1−α​∣10⟩, ψ2=α∣02⟩−1−α∣20⟩\psi_2=\sqrt\alpha|02\rangle-\sqrt{1-\alpha}|20\rangleψ2​=α​∣02⟩−1−α​∣20⟩, and ρ(α)=(∣ψ1⟩⟨ψ1∣+∣ψ2⟩⟨ψ2∣)/2\rho^{(\alpha)}=(|\psi_1\rangle\langle\psi_1|+|\psi_2\rangle\langle\psi_2|)/2ρ(α)=(∣ψ1​⟩⟨ψ1​∣+∣ψ2​⟩⟨ψ2​∣)/2. With EWE_WEW​ the infimum of log⁡2∥XTB∥1\log_2\|X^{T_B}\|_1log2​∥XTB​∥1​ over Hermitian X≥ρX\ge\rhoX≥ρ, and EηE_\etaEη​ the support-sandwich lower bound, the explicit estimates are

EW(ρ(α))≤log⁡2∥(ρ(α))TB∥1=log⁡2(1+2α(1−α)),Eη(ρ(α))≥−log⁡2(1−α).E_W(\rho^{(\alpha)})\le\log_2\|(\rho^{(\alpha)})^{T_B}\|_1=\log_2(1+\sqrt{2\alpha(1-\alpha)}),\qquad E_\eta(\rho^{(\alpha)})\ge-\log_2(1-\alpha).EW​(ρ(α))≤log2​∥(ρ(α))TB​∥1​=log2​(1+2α(1−α)​),Eη​(ρ(α))≥−log2​(1−α).

Moreover,

log⁡2(1+2α(1−α))<−log⁡2(1−α),ED(ρ(α))≤EW(ρ(α))<Eη(ρ(α))≤EC(ρ(α)).\log_2(1+\sqrt{2\alpha(1-\alpha)})<-\log_2(1-\alpha),\qquad E_D(\rho^{(\alpha)})\le E_W(\rho^{(\alpha)})<E_\eta(\rho^{(\alpha)})\le E_C(\rho^{(\alpha)}).log2​(1+2α(1−α)​)<−log2​(1−α),ED​(ρ(α))≤EW​(ρ(α))<Eη​(ρ(α))≤EC​(ρ(α)).

The decimal endpoints are exact rationals. Below α=1/2\alpha=1/2α=1/2 this family need not be antisymmetric.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P90
Formal statement
noncomputable section

open scoped Matrix ComplexConjugate ComplexOrder

namespace QAlgorithms.Papers.Independent.Intakethird100.P90

attribute [local instance] Classical.propDecidable Classical.decEq

open QAlgorithms

open QAlgorithms.Papers.Independent.Dependency50.P36
  (relativeEntropy rains target canonicalMatrix allowed pptDistillable)

open QAlgorithms.Papers.Independent.Information100.P04 (gamma copies IsPPT)

open QAlgorithms.Papers.Independent.Next46.P42 (regroupProduct)

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

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

open QAlgorithms.Papers.Independent.Gap48.P32 (antisymmetricQutrit)

/-- arXiv:1606.09421v3, PDF pp.4--5: exact rational parameter interval,
both explicit estimates, the trace-norm evaluation, and the full irreversibility chain. -/
theorem alpha_family_irreversibility (alpha : ℝ)
    (hlower : (21/50 : ℝ) ≤ alpha) (hupper : alpha ≤ (1/2 : ℝ)) :
    wangDuanBound (alphaState alpha) ≤ Real.logb 2 (1 + Real.sqrt (2*alpha*(1-alpha))) ∧
    traceNorm (gamma (alphaState alpha)) = 1 + Real.sqrt (2*alpha*(1-alpha)) ∧
    -Real.logb 2 (1-alpha) ≤ etaEntanglement (alphaState alpha) ∧
    Real.logb 2 (1 + Real.sqrt (2*alpha*(1-alpha))) < -Real.logb 2 (1-alpha) ∧
    pptDistillable (alphaState alpha) ≤ (wangDuanBound (alphaState alpha) : EReal) ∧
    wangDuanBound (alphaState alpha) < etaEntanglement (alphaState alpha) ∧
    (etaEntanglement (alphaState alpha) : EReal) ≤ asymptoticEntanglementCost false (alphaState alpha) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P90

end
Source
Irreversibility of Asymptotic Entanglement Manipulation Under Quantum Operations Completely Preserving Positivity of Partial Transpose, arXiv:1606.09421v3, PDF p. 5, Unnumbered family result: explicit irreversibility for 0.42<=alpha<=0.5
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every real α\alphaα with 2150≤α≤12\frac{21}{50}\le\alpha\le\frac125021​≤α≤21​, let ρα=12(v1v1†+v2v2†)\rho_\alpha=\frac12(v_1v_1^\dagger+v_2v_2^\dagger)ρα​=21​(v1​v1†​+v2​v2†​) on C3⊗C3\mathbb C^3\otimes\mathbb C^3C3⊗C3, where vj=α ∣0,j⟩−1−α ∣j,0⟩v_j=\sqrt{\alpha}\,|0,j\rangle-\sqrt{1-\alpha}\,|j,0\ranglevj​=α​∣0,j⟩−1−α​∣j,0⟩ for j=1,2j=1,2j=1,2. Write ΓX\Gamma XΓX for the partial transpose with entries (ΓX)(a,b),(c,d)=X(a,d),(c,b)(\Gamma X)_{(a,b),(c,d)}=X_{(a,d),(c,b)}(ΓX)(a,b),(c,d)​=X(a,d),(c,b)​, and ∥X∥1=Re⁡Tr⁡X†X\|X\|_1=\operatorname{Re}\operatorname{Tr}\sqrt{X^\dagger X}∥X∥1​=ReTrX†X​. Define W(ρ)W(\rho)W(ρ) as the infimum of log⁡2∥ΓX∥1\log_2\|\Gamma X\|_1log2​∥ΓX∥1​ over Hermitian XXX satisfying X−ρ⪰0X-\rho\succeq0X−ρ⪰0. Let PρP_\rhoPρ​ be the matrix obtained by applying the scalar function t↦0t\mapsto0t↦0 if t=0t=0t=0, and t↦1t\mapsto1t↦1 otherwise, to ρ\rhoρ by continuous functional calculus; define η(ρ)\eta(\rho)η(ρ) as the infimum of ∥ΓY∥op\|\Gamma Y\|_{\mathrm{op}}∥ΓY∥op​ over Hermitian YYY with Y−ΓPρ⪰0Y-\Gamma P_\rho\succeq0Y−ΓPρ​⪰0 and Y+ΓPρ⪰0Y+\Gamma P_\rho\succeq0Y+ΓPρ​⪰0, and define Eη(ρ)=−log⁡2η(ρ)E_\eta(\rho)=-\log_2\eta(\rho)Eη​(ρ)=−log2​η(ρ). Here a PPT channel is a map Φ\PhiΦ such that both Φ\PhiΦ and Γ∘Φ∘Γ\Gamma\circ\Phi\circ\GammaΓ∘Φ∘Γ admit finite Kraus representations Φ(X)=∑jKjXKj†\Phi(X)=\sum_jK_jXK_j^\daggerΦ(X)=∑j​Kj​XKj†​ with ∑jKj†Kj=I\sum_jK_j^\dagger K_j=I∑j​Kj†​Kj​=I. Let DPPT(ρ)D_{\mathrm{PPT}}(\rho)DPPT​(ρ) be the supremum, in the extended real numbers, of nonnegative real rates rrr such that, for every tolerance τ>0\tau>0τ>0, all sufficiently large natural nnn admit a PPT channel taking ρ⊗n\rho^{\otimes n}ρ⊗n within trace norm τ\tauτ of Ω⌈2nr⌉\Omega_{\lceil2^{nr}\rceil}Ω⌈2nr⌉​; let CPPT(ρ)C_{\mathrm{PPT}}(\rho)CPPT​(ρ) be the extended-real infimum of nonnegative real rates rrr such that, for every ε,δ>0\varepsilon,\delta>0ε,δ>0, all sufficiently large positive nnn admit a natural m≤n(r+δ)m\le n(r+\delta)m≤n(r+δ) and a PPT channel taking Ω2m\Omega_{2^m}Ω2m​ within trace norm ε\varepsilonε of ρ⊗n\rho^{\otimes n}ρ⊗n. Tensor-power basis indices are relabelled by the specified finite-set bijections, and (Ωk)(a,b),(c,d)=1/k(\Omega_k)_{(a,b),(c,d)}=1/k(Ωk​)(a,b),(c,d)​=1/k when a=ba=ba=b and c=dc=dc=d, and is zero otherwise; m=0m=0m=0 and rate r=0r=0r=0 are allowed. The assertion is

W(ρα)≤log⁡2 ⁣(1+2α(1−α)),∥Γρα∥1=1+2α(1−α),−log⁡2(1−α)≤Eη(ρα),log⁡2 ⁣(1+2α(1−α))<−log⁡2(1−α),DPPT(ρα)≤W(ρα),W(ρα)<Eη(ρα),Eη(ρα)≤CPPT(ρα),\begin{aligned} W(\rho_\alpha)&\le \log_2\!\left(1+\sqrt{2\alpha(1-\alpha)}\right),\\ \|\Gamma\rho_\alpha\|_1&=1+\sqrt{2\alpha(1-\alpha)},\\ -\log_2(1-\alpha)&\le E_\eta(\rho_\alpha),\\ \log_2\!\left(1+\sqrt{2\alpha(1-\alpha)}\right)&<-\log_2(1-\alpha),\\ D_{\mathrm{PPT}}(\rho_\alpha)&\le W(\rho_\alpha),\\ W(\rho_\alpha)&<E_\eta(\rho_\alpha),\\ E_\eta(\rho_\alpha)&\le C_{\mathrm{PPT}}(\rho_\alpha), \end{aligned}W(ρα​)∥Γρα​∥1​−log2​(1−α)log2​(1+2α(1−α)​)DPPT​(ρα​)W(ρα​)Eη​(ρα​)​≤log2​(1+2α(1−α)​),=1+2α(1−α)​,≤Eη​(ρα​),<−log2​(1−α),≤W(ρα​),<Eη​(ρα​),≤CPPT​(ρα​),​

where real quantities in extended-real inequalities are embedded into the extended real numbers.

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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