Separable states have zero distillable key
ProvedHorodeckiBoundKey.separable_no_keybound-entanglementcryptographyp2o-gran-per-chapterp2o-plan-paperp2o-v1quantum-information
Let be a matrix on shared by Alice and Bob. If is a separable state, then
The paper does not state this separately. It follows from its Theorem 2, (p.4, proof in [18]), since the relative entropy of entanglement vanishes on separable states, and it is what turns into entanglement in the summary "One can even have for bound entangled states" (p.4). It gives the clause "not separable" of the main result.
Formalization Note Separability is IsSeparable. is the operational private-dit rate Gap48.P42.distillableKey, valued in . Theorem 2 itself is not posed in this mission.
Differences from the source:
- reading: the implicit claim that a state with K_D > 0 is entangled (consequence of Theorem 2, p.4) → every separable finite bipartite state has K = 0; reason: the consequence of K_D ≤ E_r^∞ with E_r = 0 on separable states, stated for every finite bipartite state as Theorem 2 is
- reading: distillable key K_D (key drawn by local operations and public communication; not defined formally in the paper) → K_γ, the operational private-dit rate Gap48.P42.distillableKey under deterministic finite adaptive LOCC (ℝ≥0∞); reason: p.2 identifies the two rates ("We thus have equality of the two rates", with "Clearly K_γ ≤ K_D") and the proof on p.3 distils γ states "at the same rate as K_D"; the mission uses this one key rate throughout
Preamble
import Mathlib import Definitions.Def_QAlgorithms_Papers_Independent_Dependency50_P24 import Definitions.Def_QAlgorithms_Papers_Independent_Gap48_P42 import Definitions.Def_HorodeckiBoundKey_IsSeparable open QAlgorithms QAlgorithms.Papers.Independent open QAlgorithms.Papers.Independent.Information100.P21 (Op) open scoped Matrix ComplexOrder ENNReal open QAlgorithms.Papers.Independent.Gap48.P42 (distillableKey)
Formal statement
namespace HorodeckiBoundKey
/-- Horodecki, Horodecki, Horodecki, Oppenheim, arXiv:quant-ph/0309110v2, p.4 ("In summary, we
have found that in general E_D ≤ K_D ≤ E_r^∞ ≤ E_c"), with p.1 ("bound entangled states (states
which require entanglement to create …)"): a separable state has zero distillable key. The
paper does not state this separately; it is the consequence of Theorem 2 (`K_D ≤ E_r^∞`, p.4,
proved in [18]) with `E_r = 0` on separable states, and it is what makes a state with positive
key entangled. Theorem 2 itself is not posed in this mission. Stated for every finite bipartite
state.
**Formalization Note.** A matrix on `Fin a × Fin b` (Alice × Bob); separability is
`IsSeparable` (finite convex combination of product density matrices). Distillable key is read
as `K_γ` (p.2): the operational rate `Gap48.P42.distillableKey` of distilling private dits by
deterministic finite adaptive LOCC, with key dimension and shields free at every blocklength,
vanishing full trace-norm error, as an `ℝ≥0∞` supremum. -/
theorem separable_no_key {a b : ℕ} (ρ : Matrix (Fin a × Fin b) (Fin a × Fin b) ℂ)
(hsep : IsSeparable ρ) : distillableKey ρ = 0 := by sorry
end HorodeckiBoundKey
Source
Horodecki, Horodecki, Horodecki, Oppenheim, Secure key from bound entanglement, arXiv:quant-ph/0309110v2, p.4 ("In summary, we have found that in general E_D ≤ K_D ≤ E_r^∞ ≤ E_c"), with Theorem 2, p.4, and p.1 ("states which require entanglement to create")
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.