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Atlas.DifferentialAnalysis.code.ConvolutionSchwartzDeriv

The shifted Peetre weight y ↦ (1 + ‖x₀ - y‖)^{-(n+1)} is Lebesgue integrable on EuclideanSpace ℝ (Fin n).

theorem ConvolutionDensity.schwartz_norm_le_of_mem_ball {n : } (φ : SchwartzMap (EuclideanSpace (Fin n)) (EuclideanSpace (Fin n) →L[] )) (x₀ x y : EuclideanSpace (Fin n)) (hx : x Metric.ball x₀ 1) :
φ (x - y) ((SchwartzMap.seminorm 0 0) φ + (SchwartzMap.seminorm (n + 1) 0) φ) * 3 ^ (n + 1) * (1 + x₀ - y) ^ (-(n + 1))

Peetre-type bound for a derivative-valued Schwartz function: for x in the unit ball around x₀, the norm of φ(x - y) is bounded by C · (1 + ‖x₀ - y‖)^{-(n+1)} with C expressed in terms of the Schwartz seminorms of φ.

theorem ConvolutionDensity.schwartz_norm_le_of_mem_ball_gen {n : } {F : Type u_1} [NormedAddCommGroup F] [NormedSpace F] (φ : SchwartzMap (EuclideanSpace (Fin n)) F) (x₀ x y : EuclideanSpace (Fin n)) (hx : x Metric.ball x₀ 1) :
φ (x - y) ((SchwartzMap.seminorm 0 0) φ + (SchwartzMap.seminorm (n + 1) 0) φ) * 3 ^ (n + 1) * (1 + x₀ - y) ^ (-(n + 1))

Generic Peetre-type bound for a Schwartz function valued in an arbitrary normed space F: for x in the unit ball around x₀, ‖φ(x - y)‖ is bounded by C · (1 + ‖x₀ - y‖)^{-(n+1)} with C expressed in terms of Schwartz seminorms of φ.

The smul-convolution x ↦ ∫ v(y) • ψ(x - y) dy of a C₀ function v with a Schwartz function ψ valued in F is Fréchet-differentiable at every x₀, with derivative given by differentiating under the integral sign.

The smul-convolution x ↦ ∫ v(y) • ψ(x - y) dy of a C₀ function v with a Schwartz function ψ valued in F is Cᵏ for every natural number k.

The convolution (v ⋆ ψ)(x) = ∫ v(y) ψ(x - y) dy of a C₀ function v with a complex-valued Schwartz function ψ is C^∞ (Melrose Prop. 8.1, smoothness part).

The cocompact filter on EuclideanSpace ℝ (Fin n) is countably generated, with complements of closed balls of integer radii as a basis.

The convolution (v ⋆ ψ)(x) = ∫ v(y) ψ(x - y) dy of a C₀ function v with a Schwartz function ψ vanishes at infinity (Melrose Prop. 8.1, decay part).

Melrose's Proposition 8.1: the convolution of a C₀ function with a Schwartz function is smooth and vanishes at infinity.