(p.3)
ProvedIsotropicSpin.norm_ZZ_YYinformation-theoryminimum-output-entropyp2o-gran-per-chapterp2o-plan-paperp2o-strengthenedp2o-v1quantum-channelsquantum-information
Let be the spin-1 matrices (13). Then
- for all real , the matrix of (19) satisfies ;
- for every unit vector , the matrix of (18) satisfies ,
where is the operator norm. With (17), this proves the bound (16) and hence (14).
Formalization Note The norm is the operator norm induced by the Euclidean norm on .
Differences from the source:
- generalization: Z of (19) with α ∈ [0, π] from (18) → every real α and β; reason: the identity holds for every α; specializes to α ∈ [0, π]
- encoding: operator norm ‖·‖ → the operator norm induced by the Euclidean norm on ℂ³ (scope Matrix.Norms.L2Operator); reason: the page says "operator norm" (p.2, before (16)); this is that norm
Preamble
import Mathlib import Definitions.Def_WHAdditivity_Renyi_Model import Definitions.Def_IsotropicSpin_spinOne import Definitions.Def_IsotropicSpin_yMat import Definitions.Def_IsotropicSpin_zMat open scoped Matrix Matrix.Norms.L2Operator
Formal statement
namespace IsotropicSpin
/-- **The norms `‖ZZ†‖ = ‖YY†‖ = 1`**, Alicki, arXiv:quant-ph/0402080v1, §2, proof of Theorem 1,
p. 3 (after (21)): "Because ZZ† is a positive matrix with trace equal 2 than it follows that its
norm ‖ZZ†‖ = ‖YY†‖ = 1".
1. `‖Z Z†‖ = 1` for all real `α, β`, with `Z` of (19);
2. `‖Y Y†‖ = 1` for every unit vector `ξ ∈ ℂ³`, with `Y = Σ_k ξ_k S_k` of (18).
**Formalization Note** `‖·‖` is the operator norm induced by the Euclidean norm
(`Matrix.Norms.L2Operator`). -/
theorem norm_ZZ_YY :
(∀ α β : ℝ, ‖zMat α β * (zMat α β)ᴴ‖ = 1) ∧
(∀ ξ : Fin 3 → ℂ, WHAdditivity.Renyi.IsUnitVector ξ → ‖yMat ξ * (yMat ξ)ᴴ‖ = 1) := by sorry
end IsotropicSpin
Source
Alicki, Isotropic quantum spin channels and additivity questions, arXiv:quant-ph/0402080v1, §2, proof of Theorem 1, sentence after (21), p.3
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.