OAI/Analysis/OInfinity/CanonicalBufferAbsorption.lean
2 declarations, 0 contain sorry, 0 declared as axioms
Absorbing a commuting canonical row into the actual vacuum split
The corner and its connected anchor come from the source row itself. The finite target completion is used only at the auxiliary index. The original source representation remains explicitly on the complementary corner.
- lemma
OAI.WeakPureInfiniteness.BufferAbsorptionCorner.exists_proper_vacuum_absorptionline 21Source documentation
A vacuum corner absorbs a proper target prefix. No commutation of the corner with the source row is required.
lemma BufferAbsorptionCorner.exists_proper_vacuum_absorption (D : BufferAbsorptionCorner E) (s t : ℕ → E) (hs : ∀ i j, star (s i) * s j = if i = j then 1 else 0) (ht : ∀ i j, star (t i) * t j = if i = j then 1 else 0) (n : ℕ) (hqz : D.q * s (n + 2) = 0) (hqt : ∀ i, Commute D.q (t i)) (hat : ∀ i, Commute (star D.a) (t i)) (hbt : ∀ i, Commute (star D.b) (t i)) (ε : ℝ) (hε : 0 < ε) : ∃ U : unitary E, Joined D.anchor U ∧ ∀ i : Fin n, ‖(U : E) * s i * star (U : E) - … - lemma
OAI.WeakPureInfiniteness.exists_connected_canonical_buffer_absorptionline 119Source documentation
All geometric, coefficient-commutation and connected-anchor hypotheses are supplied by the two commuting canonical rows. The independently chosen tolerance
κcontrols the source's actual finite vacuum split.lemma exists_connected_canonical_buffer_absorption (s t : ℕ → E) (hs : ∀ i j, star (s i) * s j = if i = j then 1 else 0) (ht : ∀ i j, star (t i) * t j = if i = j then 1 else 0) (hst : bergRowsCommute s t) (n : ℕ) (κ ε : ℝ) (hκ : 0 < κ) (hε : 0 < ε) : ∃ D : BufferAbsorptionCorner E, ∃ U : unitary E, Joined (1 : unitary E) U ∧ D.q ≠ 0 ∧ (∀ i : Fin (n + 1), ‖s i * D.q - D.q * s i‖ < κ) ∧ (∀ i : Fin (n + 1), ‖D.q * s i * D.q - zeroCornerRow D.q D.a D.b n i‖ < κ) ∧ (∀ i, Commute D.q (t i) ∧ Commute D.w (t i) ∧ …Mentions: OAI.WeakPureInfiniteness.bergRowsCommute, OAI.WeakPureInfiniteness.BufferAbsorptionCorner, OAI.WeakPureInfiniteness.zeroCornerRow