Sobolev spaces (Bessel potential spaces) #
In this file we define Sobolev spaces on normed vector spaces via the Fourier transform.
These spaces are also known as Bessel potential spaces. The Bessel potential operator
besselPotential is the Fourier multiplier with the symbol x ↦ (1 + ‖x‖ ^ 2) ^ (s / 2) and a
tempered distribution u belongs to the Sobolev space H ^ {s, p} if
besselPotential E F s u can be represented by a Lp function, informally this is written as
𝓕⁻ (fun x ↦ (1 + ‖x‖ ^ 2) ^ (s / 2)) 𝓕 u ∈ Lp.
Note that the Bessel potential is the operator (1 - (2 * π) ^ (-2) • Δ) ^ (s / 2) and not
(1 - Δ) ^ (s / 2) due to the convention of the Fourier transform. This obviously does not impact
the definition of the Sobolev spaces.
Main definitions #
TemperedDistribution.besselPotential: The Bessel potential operator is the Fourier multiplier with the function(1 + ‖x‖ ^ 2) ^ (s / 2).TemperedDistribution.memSobolev: A tempered distribution lies in the Sobolev space of ordersandpifbesselPotential E F s u ∈ Lp.
Main statements #
SchwartzMap.memSobolev: Each Schwartz function belongs to every Sobolev spaceTemperedDistribution.memSobolev_two_iff_fourier: The characterization ofp = 2Sobolev functionsTemperedDistribution.MemSobolev.fourierMultiplierCLM_of_bounded: Ifuis a Sobolev function, theng • uis a Sobolev function of the same order providedgis bounded.TemperedDistribution.MemSobolev.lineDerivOp: Ifuis a Sobolev function of orders, then∂_{m} uis a Sobolev function of orders - 1.TemperedDistribution.MemSobolev.laplacian: Ifuis a Sobolev function of orders, thenΔ uis a Sobolev function of orders - 2.
References #
The Bessel potential operator is the Fourier multiplier with the function
(1 + ‖x‖ ^ 2) ^ (s / 2).
Note that due to the convention of the Fourier transform, this is the operator
(1 - (2 * π) ^ (-2) • Δ) ^ (s / 2) not (1 - Δ) ^ (s / 2).
Equations
- TemperedDistribution.besselPotential E F s = TemperedDistribution.fourierMultiplierCLM F fun (x : E) => ↑((1 + ‖x‖ ^ 2) ^ (s / 2))
Instances For
A tempered distribution f is a Sobolev function of order s if there exists an Lp function
f' such that 𝓕⁻ (1 + ‖x‖ ^ 2) ^ (s / 2) 𝓕 f = f'.
Equations
- TemperedDistribution.MemSobolev s p f = ∃ (f' : ↥(MeasureTheory.Lp F p MeasureTheory.volume)), (TemperedDistribution.besselPotential E F s) f = MeasureTheory.Lp.toTemperedDistribution f'
Instances For
Schwartz functions are in every Sobolev space.
A tempered distribution belongs to the Sobolev space of order s and p = 2 if and only if
its Fourier transform multiplied by (1 + ‖x‖ ^ 2) ^ (s / 2) is in Lp.
The Fourier transform of a Sobolev function of order s with s > d / 2 can be represented by
a L1 function.
This is the main calculation of the Sobolev embedding theorem.
The Fourier multiplier with a bounded function maps H ^ s to H ^ s.
The directional derivative maps H ^ s to H ^ {s - 1}.
The Laplacian maps H ^ s to H ^ {s - 2}.