PPT states have zero distillable entanglement ([22])
ProvedHorodeckiBoundKey.ppt_undistillableLet be a state (positive semidefinite, trace one) on , shared by Alice (first factor) and Bob (second factor). If has positive partial transpose, , then no pure entanglement can be distilled from it:
Here is the distillable entanglement: the supremum of rates such that, for every and all large , a deterministic finite LOCC protocol turns into a state within trace distance of Bell pairs with .
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 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 . is the published operational rate Gap48.P42.bipartiteDistillable, valued in .
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
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)
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
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.