OAI/NumberTheory/Ostmann/Supply/FiniteTensorKernel.lean
4 declarations, 0 contain sorry, 0 declared as axioms
Finite products of the local residue matrices
- theorem
OAI.Ostmann.kernel_energy_reindexline 13 - def
OAI.Ostmann.finiteTensorKernelline 27 - theorem
OAI.Ostmann.finiteTensorKernel_energy_leline 32Source documentation
Iterating the two-factor bound never introduces the sizes of the residue fields.
theorem finiteTensorKernel_energy_le {n : ℕ} (α : Fin n → Type u) (β : Fin n → Type v) [∀ i, Fintype (α i)] [∀ i, Fintype (β i)] (M : ∀ i, α i → β i → ℂ) (A : Fin n → ℝ) (hM : ∀ i (f : β i → ℂ), (∑ x, ‖∑ y, M i x y * f y‖ ^ 2) ≤ A i ^ 2 * ∑ y, ‖f y‖ ^ 2) (f : (∀ i, β i) → ℂ) : (∑ x, ‖∑ y, finiteTensorKernel M x y * f y‖ ^ 2) ≤ (∏ i, A i) ^ 2 * ∑ y, ‖f y‖ ^ 2 := by …Mentions: OAI.Ostmann.finiteTensorKernel
- theorem
OAI.Ostmann.finiteTensorKernel_pairingline 53Source documentation
Tensor coordinates evaluate as the product of the local kernel pairings.
theorem finiteTensorKernel_pairing {ι : Type*} [Fintype ι] {α : ι → Type u} {β : ι → Type v} [∀ i, Fintype (α i)] [∀ i, Fintype (β i)] (M : ∀ i, α i → β i → ℂ) (a : ∀ i, α i → ℂ) (b : ∀ i, β i → ℂ) : (∑ x, conj (∏ i, a i (x i)) * ∑ y, finiteTensorKernel M x y * ∏ i, b i (y i)) = ∏ i, ∑ x, conj (a i x) * ∑ y, M i x y * b i y := by …Mentions: OAI.Ostmann.finiteTensorKernel