Theorem 1, p. 2 — characterization of pure stationary states
ProvedDissipativePrep.Unique.theorem_1dissipative-state-preparationlindblad-master-equationp2o-batch-pfp2ap2o-gran-per-chapterp2o-plan-paperp2o-v1stationary-state
Let be the Liouvillian of Eq. (2) with Hermitian Hamiltonian , jump operators and rates , and write , . Let be a unit vector. Then if and only if
- for some , and
- for every , for some with
The theorem reduces stationarity of a pure state to a common-eigenvector condition on the jump operators, which is the basis of the construction in §IV.
Formalization Note The page allows ; with the operator does not enter and condition 2 can fail, so is assumed. is required to be a unit vector (a state).
Preamble
import Mathlib import Definitions.Def_DissipativePrep_Unique_Model open scoped Matrix ComplexConjugate open QAlgorithms QAlgorithms.Papers.Independent.Dependency50.P16
Formal statement
namespace DissipativePrep.Unique
theorem theorem_1 {d m : ℕ} (H : Matrix (Fin d) (Fin d) ℂ) (hH : H.IsHermitian)
(c : Fin m → Matrix (Fin d) (Fin d) ℂ) (g : Fin m → ℝ) (hg : ∀ l, 0 < g l)
(Φ : EuclideanSpace ℂ (Fin d)) (hΦ : ‖Φ‖ = 1) :
gkslGenerator (krausData H hH c g) (pureDensity Φ) = 0 ↔
∃ lam : ℂ, act (Qop H c g)ᴴ Φ = lam • Φ ∧
∃ lamL : Fin m → ℂ, (∀ l, act (c l) Φ = lamL l • Φ) ∧
∑ l, g l * ‖lamL l‖ ^ 2 = lam.re := by sorry
end DissipativePrep.Unique
Source
Kraus et al., Preparation of entangled states by quantum Markov processes, arXiv:0803.1463v3, p. 2, Theorem 1
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.