logo

Distributions, Generalized Functions 📂Distribution Theory

Distributions, Generalized Functions

Definition1 2

Let ΩRn\Omega \subset \mathbb{R}^{n} be an open set. A continuous linear functional T:D(Ω)CT : \mathcal{D}(\Omega) \to \mathbb{C} on the space of test functions is defined as a distribution. That is, a distribution is an element of the dual space of the test function space. Thus

TD T \in \mathcal{D}^{\ast}

and we call DD^{\ast} the (Schwartz) distribution space.

Explanation

The name distribution seems to be influenced by the Dirac delta function being designed to represent point masses like mass concentrated at a single point. While it directly translates to distribution, mathematicians call it a distribution. The other name, generalized function, was given because it rigorously defines concepts like the Dirac delta function, which strictly speaking are not functions. An important part in the definition of distributions is the continuity. According to the equivalence conditions for a function to be continuous, the continuity of a distribution TT means the following.

ϕjϕ    T(ϕj)T(ϕ) \phi_{j} \to \phi \implies T(\phi_{j}) \to T(\phi)

However, convergence in the space of test functions is defined a bit specially. So, if we restate the definition of a distribution specifically, it goes as follows.


A functional T:D(Ω)CT : \mathcal{D}(\Omega) \to \mathbb{C} on the space of test functions D(Ω)\mathcal{D}(\Omega) is a distribution if it is linear and continuous.

  • (a) T(aϕ+bψ)=aT(ϕ)+bT(ψ)(ϕ,ψD, a,bC)T(a\phi + b \psi ) = aT(\phi)+bT(\psi)\quad (\phi,\psi\in \mathcal{D},\ a,b\in\mathbb{C})

  • (b) ϕjϕ in D    T(ϕj)T(ϕ)\phi_{j} \to \phi \text{ in } \mathcal{D} \implies T(\phi_{j}) \to T(\phi)

Under the condition that the following are satisfied for a sequence of functions {ϕj}\left\{ \phi_{j} \right\} in D(Ω)\mathcal{D}(\Omega), we define ϕjϕ in D\phi_{j} \to \phi \text{ in } \mathcal{D}.

  • (c) There exists KΩK \Subset \Omega that satisfies supp(ϕjϕ)K j\mathrm{supp} (\phi_{j}-\phi) \subset K\quad \forall\ j.

  • (d) For each multi-index α\alpha, DαϕjD^{\alpha}\phi_{j} uniformly converges to DαϕD^{\alpha} \phi.


Following the definition of a distribution, the Dirac delta function can be defined as follows.

δa:DCϕϕ(a) \begin{align*} \delta_{a} : \mathcal{D} &\to \mathbb{C} \\ \phi &\mapsto \phi (a) \end{align*}


  1. Robert A. Adams and John J. F. Foutnier, Sobolev Space (2nd Edition, 2003), p19-20 ↩︎

  2. Gerald B. Folland, Fourier Analysis and Its Applications (1992), p306-307 ↩︎