Local modes with eigenvalue decouple
ProvedFermionModewise.kappa_zero_decouplefermionslinear-algebrap2o-gran-per-chapterp2o-plan-paperp2o-v1
Let , let , be arbitrary numbers of modes, and let
satisfy . Then .
So local modes whose Williamson eigenvalue equals are not correlated with the other side; in the pure case they end up in the vacuum.
Differences from the source:
- encoding: degeneracies g_A, g_B and λ0J_{2g} = ⊕λ0J₂ → finite mode types α, β and the Williamson form with all eigenvalues λ0; reason: relabelling only, the same matrices
Preamble
import Mathlib import Definitions.Def_FermionModewise_williamson open Matrix
Formal statement
namespace FermionModewise
/-- **Modes with eigenvalue `λ₀` decouple** (Botero–Reznik, arXiv:quant-ph/0404176v3, p.8): for
`λ = λ₀`, if `M̃_{λ₀} = [[λ₀ J_{2g_A}, K̃_{λ₀}], [−K̃_{λ₀}ᵀ, λ₀ J_{2g_B}]]` satisfies `M̃_{λ₀}² = −λ₀²`,
then `K̃_{λ₀} = 0`, whatever the degeneracies `g_A`, `g_B`.
**Formalization Note.** The mode types `α`, `β` are unrelated (the degeneracies are not
restricted). -/
theorem kappa_zero_decouple {α β : Type} [Fintype α] [DecidableEq α] [Fintype β] [DecidableEq β]
(lam0 : ℝ) (hlam0 : 0 ≤ lam0) (K : Matrix (α × Fin 2) (β × Fin 2) ℝ)
(h : Matrix.fromBlocks (williamson fun _ : α => lam0) K (-Kᵀ) (williamson fun _ : β => lam0) *
Matrix.fromBlocks (williamson fun _ : α => lam0) K (-Kᵀ) (williamson fun _ : β => lam0) =
(-(lam0 ^ 2)) • (1 : Matrix ((α × Fin 2) ⊕ (β × Fin 2)) ((α × Fin 2) ⊕ (β × Fin 2)) ℝ)) :
K = 0 := by sorry
end FermionModewise
Source
Botero–Reznik, arXiv:quant-ph/0404176v3, p.8 (after (22))
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.