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