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Mathlib.Analysis.Distribution.Sobolev

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 #

Main statements #

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).

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    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
    Instances For

      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}.