The Riemann-Lebesgue Lemma #
In this file we prove the Riemann-Lebesgue lemma, for functions on finite-dimensional real vector
spaces V: if f is a function on V (valued in a complete normed space E), then the
Fourier transform of f, viewed as a function on the dual space of V, tends to 0 along the
cocompact filter. Here the Fourier transform is defined by
fun w : StrongDual ℝ V ↦ ∫ (v : V), exp (↑(2 * π * w v) * I) • f v.
This is true for arbitrary functions, but is only interesting for L¹ functions (if f is not
integrable then the integral is zero for all w). This is proved first for continuous
compactly-supported functions on inner-product spaces; then we pass to arbitrary functions using the
density of continuous compactly-supported functions in L¹ space. Finally we generalise from
inner-product spaces to arbitrary finite-dimensional spaces, by choosing a continuous linear
equivalence to an inner-product space.
Main results #
tendsto_integral_exp_inner_smul_cocompact: forVa finite-dimensional real inner product space andf : V → E, the functionfun w : V ↦ ∫ v : V, exp (2 * π * ⟪w, v⟫ * I) • f vtends to 0 alongcocompact V.tendsto_integral_exp_smul_cocompact: forVa finite-dimensional real vector space (endowed with its unique Hausdorff topological vector space structure), andWthe dual ofV, the functionfun w : W ↦ ∫ v : V, exp (2 * π * w v * I) • f vtends to alongcocompact W.Real.tendsto_integral_exp_smul_cocompact: special case of functions onℝ.Real.zero_at_infty_fourierIntegralandReal.zero_at_infty_vector_fourierIntegral: reformulations explicitly using the Fourier integral.
Shifting f by (1 / (2 * ‖w‖ ^ 2)) • w negates the integral in the Riemann-Lebesgue lemma.
Rewrite the Fourier integral in a form that allows us to use uniform continuity.
Riemann-Lebesgue Lemma for continuous and compactly-supported functions: the integral
∫ v, exp (-2 * π * ⟪w, v⟫ * I) • f v tends to 0 w.r.t. cocompact V. Note that this is primarily
of interest as a preparatory step for the more general result
tendsto_integral_exp_inner_smul_cocompact in which f can be arbitrary.
Riemann-Lebesgue lemma for functions on a real inner-product space: the integral
∫ v, exp (-2 * π * ⟪w, v⟫ * I) • f v tends to 0 as w → ∞.
The Riemann-Lebesgue lemma for functions on ℝ.
The Riemann-Lebesgue lemma for functions on ℝ, formulated via Real.fourierIntegral.
Riemann-Lebesgue lemma for functions on a finite-dimensional inner-product space, formulated
via dual space. Do not use -- it is only a stepping stone to
tendsto_integral_exp_smul_cocompact where the inner-product-space structure isn't required.
Riemann-Lebesgue lemma for functions on a finite-dimensional real vector space, formulated via dual space.
The Riemann-Lebesgue lemma, formulated in terms of VectorFourier.fourierIntegral (with the
pairing in the definition of fourierIntegral taken to be the canonical pairing between V and
its dual space).