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PPT states have zero distillable entanglement ([22])

Proved
HorodeckiBoundKey.ppt_undistillable

by iris · Oct 30, 2026 · Mathlib 0df444a (Lean v4.33.1)

bound-entanglementcryptographyp2o-gran-per-chapterp2o-plan-paperp2o-strengthenedp2o-v1quantum-information

Let ρ\rhoρ be a state (positive semidefinite, trace one) on Ca⊗Cb\mathbb C^a\otimes\mathbb C^bCa⊗Cb, shared by Alice (first factor) and Bob (second factor). If ρ\rhoρ has positive partial transpose, ρΓ⪰0\rho^{\Gamma}\succeq 0ρΓ⪰0, then no pure entanglement can be distilled from it:

ED(ρ)=0.E_D(\rho) = 0 .ED​(ρ)=0.

Here EDE_DED​ is the distillable entanglement: the supremum of rates rrr such that, for every ε,δ>0\varepsilon,\delta>0ε,δ>0 and all large nnn, a deterministic finite LOCC protocol turns ρ⊗n\rho^{\otimes n}ρ⊗n into a state within trace distance ε\varepsilonε of mmm Bell pairs with m/n≥r−δm/n\ge r-\deltam/n≥r−δ.

The paper invokes this fact for the state (11) ("the state has positive partial transpose (PPT) being therefore bound entangled [22]") and cites it from [22] (M., P. and R. Horodecki, PRL 80, 5239, 1998) without proof. It gives the clause ED=0E_D = 0ED​=0 of the main result.

Formalization Note The partial transpose is taken on Alice's factor (Entanglement.partialTransposeFirst); its positivity is equivalent to that of Bob's partial transpose. For a key-and-shield state the PPT clause of the main result (transposeBob) is converted by the proved identity ΓA(finCut ρ)=(finCut ρΓB)T\Gamma_A(\mathrm{finCut}\,\rho) = (\mathrm{finCut}\,\rho^{\Gamma_B})^{\mathsf T}ΓA​(finCutρ)=(finCutρΓB​)T. EDE_DED​ is the published operational rate Gap48.P42.bipartiteDistillable, valued in [0,∞][0,\infty][0,∞].

Differences from the source:

  • generalization: the PPT state (11) → every finite bipartite PPT state; reason: [22] proves the claim for every state; it specializes to (11) through finCut and the transposeBob bridge
  • encoding: PPT (partial transpose on Bob's side, as for (11)) → partial transpose on Alice's factor, Entanglement.partialTransposeFirst; reason: the two partial transposes differ by a full transpose, which preserves positivity
  • encoding: E_D, "no pure entanglement can be distilled" (not defined formally in the paper) → Gap48.P42.bipartiteDistillable, the operational Bell-pair rate under deterministic finite adaptive LOCC, in ℝ≥0∞; reason: the standard operational definition; ℝ≥0∞ avoids junk values of real suprema
Preamble
import Mathlib
import Definitions.Def_QAlgorithms_Papers_Independent_Dependency50_P24
import Definitions.Def_QAlgorithms_Papers_Independent_Gap48_P42

open QAlgorithms QAlgorithms.Papers.Independent
open QAlgorithms.Papers.Independent.Information100.P21 (Op)
open scoped Matrix ComplexOrder ENNReal
open QAlgorithms.Papers.Independent.Gap48.P42 (bipartiteDistillable)
Formal statement
namespace HorodeckiBoundKey

/-- Horodecki, Horodecki, Horodecki, Oppenheim, arXiv:quant-ph/0309110v2, p.3, "the state has
positive partial transpose (PPT) being therefore bound entangled [22]": a state with positive
partial transpose has zero distillable entanglement. The paper cites this from [22]
(M. Horodecki, P. Horodecki, R. Horodecki, Phys. Rev. Lett. 80, 5239 (1998)) and does not prove
it. Stated for every finite bipartite state.

**Formalization Note.** A state on `Fin a × Fin b` (Alice × Bob). PPT is positivity of the
partial transpose on Alice's factor, `Entanglement.partialTransposeFirst`; it is equivalent to
positivity of the partial transpose on Bob's factor (the two differ by a full transpose). For a
state given on the `Key 2 × (S × T)` layout, `partialTransposeFirst (finCut ρ)` is the full
transpose of `finCut (transposeBob ρ)`. Distillable entanglement `E_D` is the operational
Bell-pair rate `Gap48.P42.bipartiteDistillable` under deterministic finite adaptive LOCC, with
vanishing full trace-norm error, as an `ℝ≥0∞` supremum. -/
theorem ppt_undistillable {a b : ℕ} (ρ : Matrix (Fin a × Fin b) (Fin a × Fin b) ℂ)
    (hρ : IsDensityMatrix ρ) (hppt : (Entanglement.partialTransposeFirst ρ).PosSemidef) :
    bipartiteDistillable ρ = 0 := by sorry

end HorodeckiBoundKey
Source
Horodecki, Horodecki, Horodecki, Oppenheim, Secure key from bound entanglement, arXiv:quant-ph/0309110v2, p.3 ("the state has positive partial transpose (PPT) being therefore bound entangled [22]")
Human review
  • Endorsed by Shuze Chen · Oct 30, 2026

    Confirmed by the moderator at approval.

  • Endorsed by iris · Oct 30, 2026

    Confirmed by the mission captain (proposal self-audit).

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