Definition:Fourier Transform

Definition
The Fourier transform of a Lebesgue integrable function $f: \R^N \to \C$ is the function $\map \FF f: \R^N \to \C$ given by:
 * $\ds \map {\map \FF f} {\mathbf s} := \int_{\R^N} \map f {\mathbf x} e^{-2 \pi i \mathbf x \cdot s} \rd \mathbf x$

for $\mathbf s \in \R^N$.

Here, the product $\mathbf x \cdot \mathbf s$ in the exponential is the dot product of the vectors $\mathbf x$ and $\mathbf s$.

Real Function
Let $f: \R \to \R$ be a real function which is Lebesgue integrable.

Correctness of the definition
The function under the integral in the definition is Lebesgue integrable, as:
 * $\size {\map f {\mathbf x} e^{-2 \pi i \mathbf x \cdot s} } = \size {\map f {\mathbf x} }$

and $f$ is assumed to be integrable.

Also defined as
There exist several slightly different definitions of the Fourier transform which are commonly used.

They differ in the choice of the constant $2 \pi$ inside the exponential and/or a multiplicative constant before the integral.

The following definition is also very common:


 * $\ds \map \FF {\map f x} := \paren {2 \pi}^{-\frac N 2} \int_{\R^N} \map f {\mathbf x} \, e^{-i \mathbf x \cdot s} \rd \mathbf x$

for $s \in \R^N$.

Their properties are essentially the same.

By a simple change of variable one can always translate statements using one of the definitions into statements using another one.

Also see

 * Properties of Fourier Transform


 * Fourier Transform of Function in Lebesgue Space: the Fourier transform of a function in $\map {L^p} {\R^N}$ for $1 \le p \le 2$


 * Fourier Transform of Tempered Distribution: more generally on $\R^N$.