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 : V →L[ℝ] ℝ ↦ ∫ (v : V), exp (↑(2 * π * w v) * I) • f x
.
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
: forV
a finite-dimensional real inner product space andf : V → E
, the functionλ w : V, ∫ v : V, exp (2 * π * ⟪w, v⟫ * I) • f v
tends to 0 alongcocompact V
.tendsto_integral_exp_smul_cocompact
: forV
a finite-dimensional real vector space (endowed with its unique Hausdorff topological vector space structure), andW
the dual ofV
, the functionλ w : W, ∫ v : V, exp (2 * π * w v * I) • f v
tends to alongcocompact W
.Real.tendsto_integral_exp_smul_cocompact
: special case of functions onℝ
.Real.zero_at_infty_fourierIntegral
andReal.zero_at_infty_vector_fourierIntegral
: reformulations explicitly using the Fourier integral.
The integrand in the Riemann-Lebesgue lemma for f
is integrable iff f
is.
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 wrt 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 fourier_integral
taken to be the canonical pairing between V
and
its dual space).