Section IV — and for every commuting with
ProvedBoundEntGauss.S_equivalencecontinuous-variablesentanglementgaussian-statesp2o-gran-per-chapterp2o-plan-paperp2o-strengthenedp2o-v1partial-transposequantum-information
On the -mode phase space, let . Then
- ;
- for every real matrix with ,
Since is real orthogonal, and are unitarily equivalent. Hence for such the condition (equivalently ) follows from , so a covariance of the family is a ppt-covariance as soon as it is a covariance.
Differences from the source:
- generalization: the identity for the covariance matrix of the example (9) (and the family (11)), which commutes with S → the identity for every real γ with Sγ = γS; reason: the paper's "Consequently" uses only Sγ = γS; specializing γ to (9) or to γ(a,b,c,e,f) gives the printed claim
- encoding: "γ + iσ and γ − iσ̃ = S(γ + iσ)S are unitarily equivalent" → the matrix identity γ − iσ̃ = S(γ + iσ)S; reason: S is real orthogonal (S² = 1), so the identity is the unitary equivalence
- encoding: f canonical degrees of freedom, X = X_A ⊕ X_B, canonical coordinates → QuadratureIndex n ⊕ QuadratureIndex m (interleaved (x_j, p_j), Alice = Sum.inl), Fock space indexed by Occupation (Fin n) × Occupation (Fin m), for all n, m; reason: Lean representation of the same objects
Preamble
import Mathlib import Definitions.Def_BoundEntGauss_totalSigma import Definitions.Def_BoundEntGauss_sigmaTilde import Definitions.Def_BoundEntGauss_opS open QAlgorithms.Papers.Independent.Dependency50.P10 (complexify) open QAlgorithms.Papers.Independent.Frontier30.P08 (QuadratureIndex)
Formal statement
namespace BoundEntGauss
/-- **The symmetry S intertwines γ + iσ and γ − iσ̃.**
Werner, Wolf, *Bound entangled Gaussian states*, arXiv:quant-ph/0009118v1, Section IV, p. 4: "The most important symmetry in the example is the multiplication operator S
with diagonal matrix elements (1, 1, −1, −1, 1, −1, −1, 1). It satisfies Sσ + σ̃S = 0, and Sγ = γS.
Consequently, γ + iσ and γ − iσ̃ = S(γ + iσ)S are unitarily equivalent".
1. `S σ + σ̃ S = 0` for the `2 × 2`-mode `σ` and `σ̃`.
2. For every real `8 × 8` matrix `γ` with `S γ = γ S`: `γ − iσ̃ = S (γ + iσ) S`.
**Formalization Note.** Part 2 is stated for every `γ` commuting with `S`, the hypothesis the
paper's "Consequently" uses; it covers the example (9) and the family (11). -/
theorem S_equivalence :
opS * totalSigma 2 2 + sigmaTilde 2 2 * opS = 0 ∧
∀ Γ : Matrix (QuadratureIndex 2 ⊕ QuadratureIndex 2) (QuadratureIndex 2 ⊕ QuadratureIndex 2) ℝ,
opS * Γ = Γ * opS →
complexify Γ - Complex.I • complexify (sigmaTilde 2 2) =
complexify opS * (complexify Γ + Complex.I • complexify (totalSigma 2 2)) * complexify opS := by sorry
end BoundEntGauss
Source
Werner, Wolf, Bound entangled Gaussian states, arXiv:quant-ph/0009118v1, Section IV, p. 4
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.