Eqs. (22)–(23), p.13 — three sequential vertices
ProvedHardyFLocal.eq22_23_three_verticescausaloidp2o-gran-per-chapterp2o-plan-paperp2o-v1quantum-gravityquantum-informationsuperoperators
Let \k\Lambdal'',l',l${l''}\circ$_{l'}\circ$_l$_k$ with coefficients
The same coefficients give the printed form (22), a sum over of \{k''}\circ${k'}\circ$_k$.
So the matrix of a clump of three is computed from the pair table alone.
Differences from the source:
- reading: (22) prints k′ ◦ k″ ◦ k; reason: typographic; (21) and the left side of (22) are compositions
- reading: a "fiducial spanning set of superoperators", with Λ in "a real vector space" (p.9) → a basis over ℝ of the Hermiticity-preserving one-qubit maps; reason: real coefficients are what p.9 requires, and they exist for Hermiticity-preserving maps
- encoding: labels run from 1, and the first element of Ω² is 1 → labels are 0-based, and the first element of Ω² = Fin 16 is 0; reason: Lean convention; same instances
Preamble
import Mathlib import Definitions.Def_HardyFLocal_Superoperator import Definitions.Def_HardyFLocal_FiducialFamily set_option autoImplicit false
Formal statement
namespace HardyFLocal
/-- **Eqs. (22)–(23): three sequential vertices**, Hardy, arXiv:0804.0054v1, §5, eqs. (22)–(23), p.13
("It can be shown that, for three sequential vertices, …").
For all `l'', l', l`, the composite `$_{l''} ∘ $_{l'} ∘ $_l` has the unique expansion `Σ_k c_k $_k`
with `c_k = Σ_{n'} Λ^{1 n'}_{l'' l'} Λ^{1 k}_{n' l}` ((23), with `Λ = pairTable S`); and it has the
same coefficients in the printed form (22), a sum over `{1} × {1} × Ω²` of `$_{k''} ∘ $_{k'} ∘ $_k`.
**Formalization Note** Printed (22) omits one `∘` in `$_{k''} $_{k'} ∘ $_k`; it is read as a
composition. -/
theorem eq22_23_three_vertices (S : FiducialFamily) (l'' l' l : Ω) :
S.map l'' ∘ₗ S.map l' ∘ₗ S.map l =
∑ k, (∑ a, pairTable S l'' l' a * pairTable S a l k) • S.map k ∧
(∀ k, coordsOf S.map (S.map l'' ∘ₗ S.map l' ∘ₗ S.map l) k =
∑ a, pairTable S l'' l' a * pairTable S a l k) ∧
(∀ c : Ω → ℝ, S.map l'' ∘ₗ S.map l' ∘ₗ S.map l = ∑ k, c k • S.map k →
∀ k, c k = ∑ a, pairTable S l'' l' a * pairTable S a l k) ∧
S.map l'' ∘ₗ S.map l' ∘ₗ S.map l =
∑ p ∈ ({0} : Finset Ω) ×ˢ ({0} : Finset Ω) ×ˢ (Finset.univ : Finset Ω),
(∑ a, pairTable S l'' l' a * pairTable S a l p.2.2) •
(S.map p.1 ∘ₗ S.map p.2.1 ∘ₗ S.map p.2.2) := by sorry
end HardyFLocal
Source
L. Hardy, Formalism Locality in Quantum Theory and Quantum Gravity, arXiv:0804.0054v1, §5, eqs. (22)–(23), p.13
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.