Eq. (7) — three independent displacement channels expand into eight error patterns
ProvedLoockCVQEC.RepCode.eq_7displacementp2o-batch-pfp2ap2o-gran-per-chapterp2o-plan-paperp2o-strengthenedp2o-v1quantum-error-correctionstochastic-channel
Let be any three-mode Wigner function, an error probability and the displacement size (the identity holds for all real ). Applying the channel "displace by in with probability " independently to each of the three modes gives
The paper states this for the encoded state ; the expansion holds for every . Each term corresponds to one subset of erring channels, weighted by its probability.
Formalization Note The left-hand side is the composition of the three single-mode channels as defined; the shift vectors are written as ![d, 0, 0] and so on, Lean index being the paper's mode 1.
Differences from the source:
- generalization: stated for the encoded state W_enc → stated for every three-mode function W and all real γ, x̄₂; reason: the expansion is algebraic in W; W = W_enc gives the page's Eq. (7)
- encoding: modes and channels numbered 1, 2, 3 → Fin 3, Lean index j − 1 for the paper's mode j; reason: Lean convention; same instances
Preamble
import Mathlib import Definitions.Def_LoockCVQEC_RepCode_Protocol
Formal statement
namespace LoockCVQEC.RepCode
theorem eq_7 (γ d : ℝ) (W : (Fin 3 → ℝ) → (Fin 3 → ℝ) → ℝ) (x p : Fin 3 → ℝ) :
noisy γ d W x p =
(1 - γ) ^ 3 * W x p
+ γ * (1 - γ) ^ 2 * W (x - ![d, 0, 0]) p
+ γ * (1 - γ) ^ 2 * W (x - ![0, d, 0]) p
+ γ * (1 - γ) ^ 2 * W (x - ![0, 0, d]) p
+ γ ^ 2 * (1 - γ) * W (x - ![d, d, 0]) p
+ γ ^ 2 * (1 - γ) * W (x - ![d, 0, d]) p
+ γ ^ 2 * (1 - γ) * W (x - ![0, d, d]) p
+ γ ^ 3 * W (x - ![d, d, d]) p := by sorry
end LoockCVQEC.RepCode
Source
van Loock, A note on quantum error correction with continuous variables, arXiv:0811.3616v1, p. 2, Eq. (7)
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.