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{{short description|Mathematical transform that expresses a function of time as a function of frequency}}
{{distinguish|text=[[Separation of variables|Fourier method]] or Fourier's original [[sine and cosine transforms]]}}
{{Fourier transforms}}
[[File:CQT-piano-chord.png|thumb|The Fourier transform applied to the waveform of a [[C major]] [[piano]] [[chord (music)|chord]] (with logarithmic horizontal (frequency) axis). The first three peaks on the left correspond to the [[fundamental frequency|fundamental frequencies]] of the chord (C, E, G). The remaining smaller peaks are higher-frequency [[overtone]]s of the fundamental pitches.]]

In [[mathematics]], the '''Fourier transform''' ('''FT''') is an [[integral transform]] that takes a [[function (mathematics)|function]] as input and outputs another function that describes the extent to which various [[Frequency|frequencies]] are present in the original function. The output of the transform is a [[complex function|complex valued function]] of frequency. The term ''Fourier transform'' refers to both the [[Operation (mathematics)|mathematical operation]] and to this complex-valued function. When a distinction needs to be made, the output of the operation is sometimes called the [[frequency domain]] representation of the original function.{{refn|group=note|Sentence structure is often sufficient to distinguish the intended meaning: for example, "Apply the Fourier transform to [an input]" refers to the operation, whereas "The Fourier transform of [an input]" refers to its output.}} The Fourier transform is analogous to decomposing the [[sound]] of a musical [[Chord (music)|chord]] into the [[sound intensity|intensities]] of its constituent [[Pitch (music)|pitches]].

[[File:Fourier transform time and frequency domains (small).gif|class=skin-invert-image|thumb|right|The Fourier transform relates the time domain, in red, with a function in the domain of the frequency, in blue. The component frequencies, extended for the whole frequency spectrum, are shown as peaks in the domain of the frequency.]]

Functions that are localized in the [[time domain]] have Fourier transforms that are spread out across the frequency domain and vice versa, a phenomenon known as the [[#Uncertainty principle|uncertainty principle]]. The [[critical point (mathematics)|critical]] case for this principle is the [[Gaussian function]], of substantial importance in [[probability theory]] and [[statistics]] as well as in the study of physical phenomena exhibiting [[normal distribution]]  (e.g., [[diffusion]]). The Fourier transform of a Gaussian function is another Gaussian function. [[Joseph Fourier]] introduced [[sine and cosine transforms]] (which [[Sine and cosine transforms#Relation with complex exponentials|correspond to the imaginary and real components]] of the modern Fourier transform) in his study of [[heat transfer]], where Gaussian functions appear as solutions of the [[heat equation]].

The Fourier transform can be formally defined as an [[improper integral|improper]] [[Riemann integral]], making it an integral transform, although this definition is not suitable for many applications requiring a more sophisticated integration theory.{{refn|group=note|Depending on the application a [[Lebesgue integral]], [[distribution (mathematics)|distributional]], or other approach may be most appropriate.}} For example, many relatively simple applications use the [[Dirac delta function]], which can be treated formally as if it were a function, but the justification requires a mathematically more sophisticated viewpoint.{{refn|group=note|{{harvtxt|Vretblad|2000}} provides solid justification for these formal procedures without going too deeply into [[functional analysis]] or the [[distribution (mathematics)|theory of distributions]].}}

The Fourier transform can also be generalized to functions of several variables on [[Euclidean space]], sending a function of {{nowrap|3-dimensional}} "position space" to a function of {{nowrap|3-dimensional}} momentum (or a function of space and time to a function of [[4-momentum]]). This idea makes the spatial Fourier transform very natural in the study of waves, as well as in [[quantum mechanics]], where it is important to be able to represent wave solutions as functions of either position or momentum and sometimes both. In general, functions to which Fourier methods are applicable are complex-valued, and possibly [[vector-valued function|vector-valued]].{{refn|group=note|In [[relativistic quantum mechanics]] one encounters vector-valued Fourier transforms of multi-component wave functions. In [[quantum field theory]], operator-valued Fourier transforms of operator-valued functions of spacetime are in frequent use, see for example {{harvtxt|Greiner|Reinhardt|1996}}.}} Still further generalization is possible to functions on [[group (mathematics)|groups]], which, besides the original Fourier transform on [[Real number#Arithmetic|{{math|'''R'''}}]] or {{math|'''R'''<sup>''n''</sup>}}, notably includes the [[discrete-time Fourier transform]] (DTFT, group = {{math|[[integers|'''Z''']]}}), the [[discrete Fourier transform]] (DFT, group = [[cyclic group|{{math|'''Z''' mod ''N''}}]]) and the [[Fourier series]] or circular Fourier transform (group = [[circle group|{{math|''S''<sup>1</sup>}}]], the unit circle ≈ closed finite interval with endpoints identified). The latter is routinely employed to handle [[periodic function]]s. The [[fast Fourier transform]] (FFT) is an algorithm for computing the DFT.

== Definition ==

The Fourier transform of a [[Lebesgue integrable]] complex-valued function <math>f(x)</math> on the real line, is the complex valued function {{tmath| \widehat{f}(\xi) }}, defined by the integral{{sfn|ps=|Pinsky|2002|p=91}}
{{Equation box 1|title=Fourier transform
|indent=:|cellpadding=6 |border |border colour = #0073CF |background colour=#F5FFFA
|equation = {{NumBlk||
<math>\widehat{f}(\xi) = \int_{-\infty}^{\infty} f(x)\ e^{-i 2\pi \xi x}\,dx, \quad \forall \xi \in \mathbb{R}.</math> &nbsp; &nbsp;
|{{EquationRef|Eq.1}}}}
}}
When <math>f(x)</math> is (Lebesgue) integrable over the whole real line, the above integral converges for all <math>\xi\in\mathbb R</math>, and <math>\widehat{f}(\xi)</math> is a [[uniformly continuous]] function of <math>\xi</math> which decays to zero as {{tmath| \xi\to\infty }}.

However, the Fourier transform can also be defined for (generalized) functions for which the [[Lebesgue integral]] {{EquationNote|Eq.1}} does not make sense.{{sfn|ps=|Lieb|Loss|2001|pp=123–125}} Interpreting the integral [[weak topology|suitably]] (e.g. as an [[improper integral]] for [[locally integrable]] functions) extends the Fourier transform to functions that are not necessarily integrable over the whole real line. More generally, the Fourier transform also applies to [[generalized function]]s like the [[Dirac delta]] (and all other [[tempered distributions]]), in which case it is defined by duality rather than an integral.{{sfn|ps=|Gelfand|Shilov|1968|p=128}}

First introduced in [[Joseph Fourier|Fourier's]] ''Analytical Theory of Heat''.,<ref>{{harvnb|Fourier|1822|p=525}}</ref><ref>{{harvnb|Fourier|1878|p=408}}</ref><ref>{{harvnb|Jordan|1883}} proves on pp.&nbsp;216–226 the [[Fourier inversion theorem#Fourier integral theorem|Fourier integral theorem]] before studying Fourier series.</ref><ref>{{harvnb|Titchmarsh|1986|p=1}}</ref> the corresponding inversion formula for functions satisfying [[Fourier inversion theorem#Conditions on the function|sufficient regularity and decay properties]] is given by the [[Fourier inversion theorem]], i.e., 
{{equation box 1|title = Inverse transform
|indent =:|cellpadding= 6 |border |border colour = #0073CF |background colour=#F5FFFA
|equation = {{NumBlk||
<math>f(x) = \int_{-\infty}^{\infty} \widehat f(\xi)\ e^{i 2 \pi \xi x}\,d\xi,\quad \forall x \in \mathbb R.</math> &nbsp; &nbsp;
|{{EquationRef|Eq.2}}}}
}}
The functions <math>f</math> and <math>\widehat{f}</math> are referred to as a '''Fourier transform pair'''.<ref>{{harvnb|Rahman|2011|p=10}}</ref>&nbsp; A common notation for designating transform pairs is:<ref>{{harvnb|Oppenheim|Schafer|Buck|1999|p=58}}</ref>
<math display="block">f(x)\ \stackrel{\mathcal{F}}{\longleftrightarrow}\ \widehat f(\xi).</math>
For example, the Fourier transform of the delta function is the [[constant function]] {{tmath| 1 }}:
<math display="block">\delta(x)\ \stackrel{\mathcal{F}}{\longleftrightarrow}\  1.</math>

=== Angular frequency (''&omega;'') ===
When the independent variable ({{tmath| x }}) represents ''time'' (often denoted by {{tmath| t }}), the transform variable ({{tmath| \xi }}) represents [[frequency]] (often denoted by {{tmath| f }}). For example, if time has the unit [[second]], then frequency has the unit [[hertz]]. The transform variable can also be written in terms of [[angular frequency]], {{tmath|1= \omega = 2\pi \xi }}, with the unit [[radian]] per second.

The substitution <math>\xi = \tfrac{\omega}{2 \pi}</math> into {{EquationNote|Eq.1}} produces this convention, where function <math>\widehat f</math> is relabeled {{tmath| \widehat f_1 }}:
<math display="block">\begin{align}
\widehat f_3(\omega) &\triangleq  \int_{-\infty}^{\infty} f(x)\cdot e^{-i\omega x}\, dx = \widehat f_1\left(\tfrac{\omega}{2\pi}\right),\\
f(x) &= \frac{1}{2\pi} \int_{-\infty}^{\infty} \widehat f_3(\omega)\cdot e^{i\omega x}\, d\omega.
\end{align}
</math>
Unlike the {{EquationNote|Eq.1}} definition, the Fourier transform is no longer a [[unitary transformation]], and there is less symmetry between the formulas for the transform and its inverse.  Those properties are restored by splitting the <math>2 \pi</math> factor evenly between the transform and its inverse, which leads to another convention:
<math display="block">\begin{align}
\widehat f_2 (\omega) &\triangleq \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{\infty} f(x)\cdot e^{- i\omega x}\, dx = \frac{1}{\sqrt{2\pi}}\  \ \widehat f_1 \left(\tfrac{\omega}{2\pi}\right), \\
f(x) &= \frac{1}{\sqrt{2\pi}} \int_{-\infty}^{\infty} \widehat f_2 (\omega)\cdot e^{ i\omega x}\, d\omega.
\end{align}</math>
Variations of all three conventions can be created by conjugating the complex-exponential [[integral kernel|kernel]] of both the forward and the reverse transform. The signs must be opposites.

{| class="wikitable"
|+ Summary of popular forms of the Fourier transform, one-dimensional
|-
! ordinary frequency {{mvar|ξ}} (Hz)
! unitary
| <math>\begin{align}
\widehat f_1(\xi)\ &\triangleq\ \int_{-\infty}^{\infty} f(x)\, e^{-i 2\pi \xi x}\, dx = \sqrt{2\pi}\ \ \widehat f_2(2 \pi \xi) = \widehat f_3(2 \pi \xi) \\
f(x) &= \int_{-\infty}^{\infty} \widehat f_1(\xi)\, e^{i 2\pi x \xi}\, d\xi \end{align}</math>
|-
! rowspan="2" | angular frequency {{mvar|ω}} (rad/s)
! unitary
| <math>\begin{align}
\widehat f_2(\omega)\ &\triangleq\ \frac{1}{\sqrt{2\pi}}\ \int_{-\infty}^{\infty} f(x)\,  e^{-i \omega x}\, dx = \frac{1}{\sqrt{2\pi}}\ \ \widehat f_1  \! \left(\frac{\omega}{2 \pi}\right) = \frac{1}{\sqrt{2\pi}}\ \ \widehat f_3 (\omega) \\
f(x) &= \frac{1}{\sqrt{2\pi}}\ \int_{-\infty}^{\infty} \widehat f_2 (\omega)\, e^{i \omega x}\, d\omega \end{align}</math>
|-
! non-unitary
| <math>\begin{align}
\widehat f_3 (\omega) \ &\triangleq\ \int_{-\infty}^{\infty} f(x)\,  e^{-i\omega x}\, dx = \widehat f_1  \left(\frac{\omega}{2 \pi}\right) = \sqrt{2\pi}\ \ \widehat f_2 (\omega) \\
f(x) &= \frac{1}{2 \pi} \int_{-\infty}^{\infty} \widehat f_3 (\omega)\, e^{i \omega x}\, d\omega \end{align}</math>
|}

{| class="wikitable"
|+ Generalization for {{math|''n''}}-dimensional functions
|-
! ordinary frequency {{mvar|ξ}} (Hz)
! unitary
| <math>\begin{align}
\widehat f_1 (\xi)\ &\triangleq\ \int_{\mathbb{R}^n} f(x) e^{-i 2\pi \xi\cdot x}\, dx = (2 \pi)^\frac{n}{2}\widehat f_2 (2\pi \xi) = \widehat f_3 (2\pi \xi) \\
f(x) &= \int_{\mathbb{R}^n} \widehat f_1 (\xi) e^{i 2\pi \xi\cdot x}\, d\xi \end{align}</math>
|-
! rowspan="2" | angular frequency {{mvar|ω}} (rad/s)
! unitary
| <math>\begin{align}
\widehat f_2 (\omega)\ &\triangleq\ \frac{1}{(2 \pi)^\frac{n}{2}} \int_{\mathbb{R}^n} f(x) e^{-i \omega\cdot x}\, dx = \frac{1}{(2 \pi)^\frac{n}{2}} \widehat f_1  \! \left(\frac{\omega}{2 \pi}\right) = \frac{1}{(2 \pi)^\frac{n}{2}} \widehat f_3 (\omega) \\
f(x) &= \frac{1}{(2 \pi)^\frac{n}{2}} \int_{\mathbb{R}^n} \widehat f_2 (\omega)e^{i \omega\cdot x}\, d\omega \end{align}</math>
|-
! non-unitary
| <math>\begin{align}
\widehat f_3 (\omega) \ &\triangleq\ \int_{\mathbb{R}^n} f(x) e^{-i\omega\cdot x}\, dx = \widehat f_1  \left(\frac{\omega}{2 \pi}\right) = (2 \pi)^\frac{n}{2} \widehat f_2 (\omega) \\
f(x) &= \frac{1}{(2 \pi)^n} \int_{\mathbb{R}^n} \widehat f_3 (\omega) e^{i \omega\cdot x}\, d\omega \end{align}</math>
|}

=== Lebesgue integrable functions ===
{{see also|Lp space#Lp spaces and Lebesgue integrals|l1=L<sup>p</sup> space § L<sup>p</sup> spaces and Lebesgue integrals}}

A [[measurable function]] <math>f:\mathbb R\to\mathbb C</math> is called (Lebesgue) integrable if the [[Lebesgue integral]] of its [[absolute value]] is finite:
<math display="block">\|f\|_1 = \int_{\mathbb R}|f(x)|\,dx < \infty.</math>
If <math>f</math> is Lebesgue integrable then the Fourier transform, given by {{EquationNote|Eq.1}}, is well-defined for all {{tmath| \xi\in\mathbb R }}.{{sfn|ps=|Stade|2005|pp=298–299}} Furthermore, <math>\widehat f\in L^\infty\cap C_0(\mathbb R)</math> is bounded, [[uniformly continuous]] and (by the [[Riemann–Lebesgue lemma]]) [[Vanish at infinity|vanishing at infinity]]. Here <math>C_0(\mathbb R)</math> denotes the space of continuous functions on <math>\mathbb R</math> that approach 0 as x approaches positive or negative infinity.

The space <math>L^1(\mathbb R)</math> is the space of measurable functions for which the norm <math>\|f\|_1</math> is finite, modulo the [[Equivalence class|equivalence relation]] of equality [[almost everywhere]].  The Fourier transform on <math>L^1(\mathbb R)</math> is [[Bijection, injection and surjection|one-to-one]].  However, there is no easy characterization of the image, and thus no easy characterization of the inverse transform.  In particular, {{EquationNote|Eq.2}} is no longer valid, as it was stated only under the hypothesis that <math>f(x)</math> was "sufficiently nice" (e.g., <math>f(x)</math> [[Schwartz function|decays with all derivatives]]).

While {{EquationNote|Eq.1}} defines the Fourier transform for (complex-valued) functions in {{tmath| L^1(\mathbb R) }}, it is not well-defined for other integrability classes, most importantly the space of [[square-integrable function]]s {{tmath| L^2(\mathbb R) }}. For example, the function <math>f(x)=(1+x^2)^{-1/2}</math> is in <math>L^2</math> but not <math>L^1</math> and therefore the Lebesgue integral {{EquationNote|Eq.1}} does not exist. However, the Fourier transform on the dense subspace <math>L^1\cap L^2(\mathbb R) \subset L^2(\mathbb R)</math> admits a unique continuous extension to a [[unitary operator]] on {{tmath| L^2(\mathbb R) }}. This extension is important in part because, unlike the case of {{tmath| L^1 }}, the Fourier transform is an [[automorphism]] of the space {{tmath| L^2(\mathbb R) }}.

In such cases, the Fourier transform can be obtained explicitly by [[Regularization (mathematics)|regularizing]] the integral, and then passing to a limit. In practice, the integral is often regarded as an [[improper integral]] instead of a proper Lebesgue integral, but sometimes for convergence one needs to use [[weak limit]] or [[Cauchy principal value|principal value]] instead of the (pointwise) limits implicit in an improper integral. {{harvtxt|Titchmarsh|1986}} and {{harvtxt|Dym|McKean|1985}} each gives three rigorous ways of extending the Fourier transform to square integrable functions using this procedure.  A general principle in working with the <math>L^2</math> Fourier transform is that finite linear combinations of Gaussians are dense in {{tmath| L^1\cap L^2 }}, and the various features of the Fourier transform, such as its unitarity, are easily inferred for Gaussians.  Many of the  properties of the Fourier transform can then be proven from two facts about Gaussians:{{sfn|ps=|Howe|1980}}
* that <math>e^{-\pi x^2}</math> is its own Fourier transform; and
* that the [[Gaussian integral]] {{tmath|1= \textstyle \int_{-\infty}^\infty e^{-\pi x^2}\,dx = 1 }}.

A feature of the <math>L^1</math> Fourier transform is that it is a homomorphism of Banach algebras from <math>L^1</math> equipped with the convolution operation to the Banach algebra of continuous functions under the <math>L^\infty</math> (supremum) norm.  The conventions chosen in this article are those of [[harmonic analysis]], such that the Fourier transform is both [[Unitary operator|unitary]] on {{tmath|L^2}} and an algebra homomorphism from {{tmath|L^1=}} to {{tmath|L^\infty}}, without renormalizing the Lebesgue measure.<ref>{{harvnb|Folland|1989}}</ref>

== Background ==
=== History ===
{{main|Fourier analysis#History|Fourier series#History}}
In 1822, Fourier claimed (see ''{{section link|Joseph Fourier|The Analytic Theory of Heat}}'') that any function, whether continuous or discontinuous, can be expanded into a series of sines.<ref>{{harvnb|Fourier|1822}}</ref> That important work was corrected and expanded upon by others to provide the foundation for the various forms of the Fourier transform used since.

=== Complex sinusoids ===
<div class="skin-invert-image">{{multiple image
| total_width       = 300
| align             = right
| image1            = Sine voltage.svg
| image2            = Phase shift.svg
| footer            =
The red [[sine wave|sinusoid]] can be described by peak amplitude (1), peak-to-peak (2), [[root mean square|RMS]] (3), and [[wavelength]] (4). The red and blue sinusoids have a phase difference of {{mvar|θ}}.
}}</div>
In general, the coefficients <math>\widehat f(\xi)</math> are complex numbers, which have two equivalent forms (see ''[[Euler's formula]]''):
<math display="block"> \widehat f(\xi) = \underbrace{A e^{i \theta}}_{\text{polar coordinate form}}
= \underbrace{A \cos(\theta) + i A \sin(\theta)}_{\text{rectangular coordinate form}}.</math>

The product with <math>e^{i 2 \pi \xi x}</math> ({{EquationNote|Eq.2}}) has these forms:
<math display="block">\begin{aligned}\widehat f(\xi)\cdot e^{i 2 \pi \xi x}
&= A e^{i \theta} \cdot e^{i 2 \pi \xi x}\\[6pt]
&= \underbrace{A e^{i (2 \pi \xi x+\theta)}}_{\text{polar coordinate form}}\\[6pt]
&= \underbrace{A\cos(2\pi \xi x +\theta) + i A\sin(2\pi \xi x +\theta)}_{\text{rectangular coordinate form}},\end{aligned}</math>
which conveys both [[amplitude]] and [[phase offset|phase]] of frequency {{tmath| \xi }}. Likewise, the intuitive interpretation of {{EquationNote|Eq.1}} is that multiplying <math>f(x)</math> by <math>e^{-i 2\pi \xi x}</math> has the effect of subtracting <math>\xi</math> from every frequency component of function {{tmath| f(x) }}.{{refn|group=note|A possible source of confusion is the [[#Frequency shifting|frequency-shifting property]]; i.e. the transform of function <math>f(x)e^{-i 2\pi \xi_0 x}</math> is {{tmath| \widehat{f}(\xi+\xi_0) }}. The value of this function at <math>\xi=0</math> is {{tmath| \widehat{f}(\xi_0) }}, meaning that a frequency <math>\xi_0</math> has been shifted to zero (also see ''{{section link|Negative frequency#Simplifying the Fourier transform}}'').}} Only the component that was at frequency <math>\xi</math> can produce a non-zero value of the infinite integral, because (at least formally) all the other shifted components are oscillatory and integrate to zero (see ''{{section link|#Example}}'').

It is noteworthy how easily the product was simplified using the polar form, and how easily the rectangular form was deduced by an application of Euler's formula.

=== Negative frequency ===
{{see also|Negative frequency#Simplifying the Fourier transform|l1=Negative frequency § Simplifying the Fourier transform}}

Euler's formula introduces the possibility of negative {{tmath| \xi }}. {{EquationNote|Eq.1}} is defined {{tmath| \forall \xi \in \mathbb{R} }}.  Only certain complex-valued <math> f(x)</math> have transforms {{tmath|1= \widehat f =0, \ \forall \ \xi < 0 }}. (See ''[[Analytic signal]]''; a simple example is {{tmath| e^{i 2 \pi \xi_0 x}\ (\xi_0 > 0) }}.)&nbsp; But negative frequency is necessary to characterize all other complex-valued {{tmath| f(x) }}, found in [[signal processing]], [[partial differential equations]], [[radar]], [[nonlinear optics]], [[quantum mechanics]], and others.

For a real-valued {{tmath| f(x) }},  {{EquationNote|Eq.1}} has the symmetry property <math>\widehat f(-\xi) = \widehat {f}^* (\xi)</math>  (see ''{{section link|#Conjugation}}'' below). This redundancy enables {{EquationNote|Eq.2}} to distinguish <math>f(x) = \cos(2 \pi \xi_0 x)</math> from {{tmath| e^{i2 \pi \xi_0 x} }}.  But it cannot determine the actual sign of {{tmath| \xi_0 }}, because <math>\cos(2 \pi \xi_0 x)</math> and <math>\cos(2 \pi (-\xi_0) x)</math> are indistinguishable on just the real numbers line.

=== Fourier transform for periodic functions ===
The Fourier transform of a periodic function cannot be defined using the integral formula directly.  In order for integral in {{EquationNote|Eq.1}} to be defined the function must be [[Absolutely integrable function|absolutely integrable]].  Instead it is common to use [[Fourier series]].  It is possible to extend the definition to include periodic functions by viewing them as [[Distribution (mathematics)#Tempered distributions|tempered distributions]].

This makes it possible to see a connection between the [[Fourier series]] and the Fourier transform for periodic functions that have a [[Convergence of Fourier series|convergent Fourier series]].  If <math>f(x)</math> is a [[periodic function]], with period {{tmath| P }}, that has a convergent Fourier series, then:
<math display="block">
\widehat{f}(\xi) = \sum_{n=-\infty}^\infty c_n \cdot \delta \left(\xi - \tfrac{n}{P}\right),
</math>
where <math>c_n</math> are the Fourier series coefficients of {{tmath| f }}, and <math>\delta</math> is the [[Dirac delta function]].  In other words, the Fourier transform is a [[Dirac comb]] function whose ''teeth'' are multiplied by the Fourier series coefficients.

=== Sampling the Fourier transform ===
{{broader|Poisson summation formula}}
The Fourier transform of an [[Absolutely integrable function|integrable]] function <math>f</math> can be sampled at regular intervals of arbitrary length {{tmath| 1/P }}. These samples can be deduced from one cycle of a periodic function {{tmath| f_P }}, which has [[Fourier series]] coefficients proportional to those samples by the [[Poisson summation formula]]:
<math display="block">f_P(x) \triangleq \sum_{n=-\infty}^{\infty} f(x+nP) = \frac{1}{P}\sum_{k=-\infty}^{\infty} \widehat f\left(\tfrac{k}{P}\right) e^{i2\pi \frac{k}{P} x}, \quad \forall k \in \mathbb{Z} .</math>

The integrability of <math>f</math> ensures the [[periodic summation]] converges.  Therefore, the samples <math>\widehat f(\tfrac{k}{P})</math> can be determined by Fourier series analysis:
<math display="block">\widehat f\left(\tfrac{k}{P}\right) = \int_{P} f_P(x) \cdot e^{-i2\pi \frac{k}{P} x} \,dx.</math>

When <math>f(x)</math> has [[compact support]], <math>f_P(x)</math> has a finite number of terms within the interval of integration.  When <math>f(x)</math> does not have compact support, numerical evaluation of <math>f_P(x)</math> requires an approximation, such as tapering <math>f(x)</math> or truncating the number of terms.

== Units ==
{{see also|Spectral density#Units}}

The frequency variable must have inverse units to the units of the original function's domain (typically named <math>t</math> or {{tmath| x }}). For example, if <math>t</math> is measured in seconds, <math>\xi</math> should be in cycles per second or [[hertz]]. If the scale of time is in units of <math>2\pi</math> seconds, then another Greek letter <math>\omega</math> is typically used instead to represent [[angular frequency]] (where {{tmath|1= \omega=2\pi \xi }}) in units of [[radian]]s per second. If using <math>x</math> for units of length, then <math>\xi</math> must be in inverse length, e.g., [[wavenumber]]s. That is to say, there are two versions of the real line: one that is the [[Range of a function|range]] of <math>t</math> and measured in units of {{tmath| t }}, and the other that is the range of <math>\xi</math> and measured in inverse units to the units of {{tmath| t }}. These two distinct versions of the real line cannot be equated with each other. Therefore, the Fourier transform goes from one space of functions to a different space of functions: functions that have a different domain of definition.

In general, <math>\xi</math> must always be taken to be a [[linear form]] on the space of its domain, which is to say that the second real line is the [[dual space]] of the first real line. (See the article ''[[Linear algebra]]'' for a more formal explanation and for more details.) This point of view becomes essential in generalizations of the Fourier transform to general [[symmetry group]]s, including the case of Fourier series.

That there is no one preferred way (often, one says "no canonical way") to compare the two versions of the real line that are involved in the Fourier transform—fixing the units on one line does not force the scale of the units on the other line—is the reason for the plethora of rival conventions on the definition of the Fourier transform. The various definitions resulting from different choices of units differ by various constants.

In other conventions, the Fourier transform has {{mvar|i}} in the exponent instead of {{math|−''i''}}, and vice versa for the inversion formula. This convention is common in modern physics<ref>{{harvnb|Arfken|1985}}</ref> and is the default for [https://www.wolframalpha.com Wolfram Alpha], and does not mean that the frequency has become negative, since there is no canonical definition of positivity for frequency of a complex wave. It simply means that <math>\widehat f(\xi)</math> is the amplitude of the wave&nbsp;{{tmath| e^{-i 2\pi \xi x} }} instead of the wave&nbsp;<math>e^{i 2\pi \xi x}</math> (the former, with its minus sign, is often seen in the time dependence for [[sinusoidal plane-wave solutions of the electromagnetic wave equation]], or in the [[Wave function#Time dependence|time dependence for quantum wave functions]]). Many of the identities involving the Fourier transform remain valid in those conventions, provided all terms that explicitly involve {{math|''i''}} have it replaced by {{math|−''i''}}.  In [[electrical engineering]] the letter {{math|''j''}} is typically used for the [[imaginary unit]] instead of {{math|''i''}} because {{math|''i''}} is used for current.

When using [[dimensionless units]], the constant factors might not be written in the transform definition. For instance, in [[probability theory]], the characteristic function {{mvar|Φ}} of the probability density function {{tmath|f}} of a random variable {{tmath|X}} of continuous type is defined without a negative sign in the exponential, and since the units of {{tmath|x}} are ignored, there is no {{tmath|2\pi}} either:
<math display="block">\varphi (\lambda) = \int_{-\infty}^\infty f(x) e^{i\lambda x} \,dx.</math>

In probability theory and mathematical statistics, the use of the Fourier—Stieltjes transform is preferred, because many random variables are not of continuous type, and do not possess a density function, and one must treat not functions but [[Distribution (mathematics)|distributions]], i.e., measures that possess "atoms".

From the higher point of view of [[character theory|group characters]], which is much more abstract, all these arbitrary choices disappear, as will be explained in the later section of this article, which treats the notion of the Fourier transform of a function on a [[locally compact abelian group]].

== Properties ==

Let <math>f(x)</math> and <math>h(x)</math> represent ''integrable functions'' [[Lebesgue-measurable]] on the real line satisfying:
<math display="block">\int_{-\infty}^\infty |f(x)| \, dx < \infty.</math>
We denote the Fourier transforms of these functions as <math>\widehat f(\xi)</math> and <math>\widehat h(\xi)</math> respectively.

=== Basic properties ===
The Fourier transform has the following basic properties:<ref name="Pinsky-2002">{{harvnb|Pinsky|2002}}</ref>

==== Linearity ====

<math display="block">a\ f(x) + b\ h(x)\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ a\ \widehat f(\xi) + b\ \widehat h(\xi);\quad \ a,b \in \mathbb C</math>

==== Time shifting ====

<math display="block">f(x-x_0)\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ e^{-i 2\pi x_0 \xi}\ \widehat f(\xi);\quad \ x_0 \in \mathbb R</math>

==== Frequency shifting ====

<math display="block">e^{i 2\pi \xi_0 x} f(x)\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ \widehat f(\xi - \xi_0);\quad \ \xi_0 \in \mathbb R</math>

==== Time scaling ====

<math display="block">f(ax)\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ \frac{1}{|a|}\widehat{f}\left(\frac{\xi}{a}\right);\quad \ a \ne 0 </math>
The case <math>a=-1</math> leads to the ''time-reversal property'':
<math display="block">f(-x)\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ \widehat f (-\xi)</math>

<div class="skin-invert">{{annotated image
| caption=The transform of an even-symmetric real-valued function {{tmath|1= f(t) = f_{_{\text{RE} } } }} is also an even-symmetric real-valued function ({{tmath| \widehat f\!_{_{\text{RE} } } }}).  The time-shift, {{tmath|1= g(t) = g_{_{\text{RE} } } + g_{_{\text{RO} } } }}, creates an imaginary component, {{tmath| i\ \widehat{g\ \!}_{_{\text{IO} } } }}.  (See ''{{section link|#Symmetry}}''.)
| image=Fourier_unit_pulse.svg
| image-width = 300
| outer-css = color: black;
| annotations =
{{annotation|20|40|<math>\scriptstyle f(t)</math>}}
{{annotation|170|40|<math>\scriptstyle \widehat{f}(\omega)</math>}}
{{annotation|20|140|<math>\scriptstyle g(t)</math>}}
{{annotation|170|140|<math>\scriptstyle \widehat{g}(\omega)</math>}}
{{annotation|130|80|<math>\scriptstyle t</math>}}
{{annotation|280|85|<math>\scriptstyle \omega</math>}}
{{annotation|130|192|<math>\scriptstyle t</math>}}
{{annotation|280|180|<math>\scriptstyle \omega</math>}}
}}</div>

==== Symmetry ====
When the real and imaginary parts of a complex function are decomposed into their [[Even and odd functions#Even–odd decomposition|even and odd parts]], there are four components, denoted below by the subscripts RE, RO, IE, and IO.  And there is a one-to-one mapping between the four components of a complex time function and the four components of its complex frequency transform:{{sfn|ps=|Proakis|Manolakis|1996|p=[https://archive.org/details/digitalsignalpro00proa/page/291 291]}}
: <math>
\begin{array}{rlcccccccc}
\mathsf{Time\ domain} & f & = & f_{_{\text{RE}}} & + & f_{_{\text{RO}}} & + & i\ f_{_{\text{IE}}} & + & \underbrace{i\ f_{_{\text{IO}}}} \\
&\Bigg\Updownarrow\mathcal{F} & &\Bigg\Updownarrow\mathcal{F} & &\ \ \Bigg\Updownarrow\mathcal{F} & &\ \ \Bigg\Updownarrow\mathcal{F} & &\ \ \Bigg\Updownarrow\mathcal{F}\\
\mathsf{Frequency\ domain} & \widehat f & = & \widehat f\!_{_{\text{RE}}} & + & \overbrace{i\ \widehat f\!_{_{\text{IO}}}} & + & i\ \widehat f\!_{_{\text{IE}}} & + & \widehat f\!_{_{\text{RO}}}
\end{array}
</math>

From this, various relationships are apparent, for example:
* The transform of a real-valued function ({{tmath| f_{_{\text{RE} } }+f_{_{\text{RO} } } }}) is the ''[[Even and odd functions#Complex-valued functions|conjugate symmetric]]'' function {{tmath| \widehat f\!_{_{\text{RE} } }+i\ \widehat f\!_{_{\text{IO} } } }}.  Conversely, a ''conjugate symmetric'' transform implies a real-valued time-domain.
* The transform of an imaginary-valued function ({{tmath| i\ f_{_{\text{IE} } }+i\ f_{_{\text{IO} } } }}) is the ''[[Even and odd functions#Complex-valued functions|conjugate antisymmetric]]'' function {{tmath| \widehat f\!_{_{\text{RO} } }+i\ \widehat f\!_{_{\text{IE} } } }}, and the converse is true.
* The transform of a ''[[Even and odd functions#Complex-valued functions|conjugate symmetric]]'' function <math>(f_{_{\text{RE}}}+i\ f_{_{\text{IO}}})</math> is the real-valued function {{tmath| \widehat f\!_{_{\text{RE} } }+\widehat f\!_{_{\text{RO} } } }}, and the converse is true.
* The transform of a ''[[Even and odd functions#Complex-valued functions|conjugate antisymmetric]]'' function <math>(f_{_{\text{RO}}}+i\ f_{_{\text{IE}}})</math> is the imaginary-valued function {{tmath| i\ \widehat f\!_{_{\text{IE} } }+i\ \widehat f\!_{_{\text{IO} } } }}, and the converse is true.

==== Conjugation ====
<math display="block">\bigl(f(x)\bigr)^*\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ \left(\widehat{f}(-\xi)\right)^*</math>
(Note: the {{tmath|*}} denotes [[Complex conjugate|complex conjugation]].)

In particular, if <math>f</math> is ''real'', then <math>\widehat f</math> is [[Even and odd functions#Complex-valued functions|conjugate symmetric]] ({{aka}} [[Hermitian function]]):
<math display="block">\widehat{f}(-\xi)=\bigl(\widehat f(\xi)\bigr)^*.</math>

If <math>f</math> is purely imaginary, then <math>\widehat f</math> is [[Even and odd functions#Complex-valued functions|odd symmetric]]:
<math display="block">\widehat f(-\xi) = -(\widehat f(\xi))^*.</math>

==== Real and imaginary parts ====
<math display="block">\operatorname{Re}\{f(x)\}\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ 
\tfrac{1}{2} \left( \widehat f(\xi) + \bigl(\widehat f (-\xi) \bigr)^* \right)</math>
<math display="block">\operatorname{Im}\{f(x)\}\ \ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \ 
\tfrac{1}{2i} \left( \widehat f(\xi) - \bigl(\widehat f (-\xi) \bigr)^* \right)</math>

==== Zero frequency component ====
Substituting <math>\xi = 0</math> in the definition, we obtain:
<math display="block">\widehat{f}(0) = \int_{-\infty}^{\infty} f(x)\,dx.</math>

The integral of <math>f</math> over its domain is the total mass or [[DC bias]] of the function.

=== Uniform continuity and the Riemann–Lebesgue lemma ===
[[File:Rectangular function.svg|class=skin-invert-image|thumb|The [[rectangular function]] is [[Lebesgue integrable]].]]
[[File:Sinc function (normalized).svg|class=skin-invert-image|thumb|The [[sinc function]], which is the Fourier transform of the rectangular function, is bounded and continuous, but not Lebesgue integrable.]]
The Fourier transform may be defined in some cases for non-integrable functions, but the Fourier transforms of integrable functions have several strong properties.

The Fourier transform <math>\widehat{f}</math> of any integrable function <math>f</math> is [[uniformly continuous]] and{{sfn|ps=|Katznelson|2004|p=153}}{{sfn|ps=|Stein|Weiss|1971|p=2}}
<math display="block">\left\|\widehat{f}\right\|_\infty \leq \left\|f\right\|_1</math>

By the ''[[Riemann–Lebesgue lemma]]'',<ref name="Stein-Weiss-1971">{{harvnb|Stein|Weiss|1971}}</ref>
<math display="block">\widehat{f}(\xi) \to 0\text{ as }|\xi| \to \infty.</math>

However, <math>\widehat{f}</math> need not be integrable. For example, the Fourier transform of the [[rectangular function]], which is integrable, is the [[sinc function]], which is not [[Lebesgue integrable]], because its [[improper integral]]s behave analogously to the [[alternating harmonic series]], in converging to a sum without being [[absolutely convergent]].

It is not generally possible to write the ''inverse transform'' as a [[Lebesgue integral]]. However, when both <math>f</math> and <math>\widehat{f}</math> are integrable, the inverse equality
<math display="block">f(x) = \int_{-\infty}^\infty \widehat f(\xi) e^{i 2\pi x \xi} \, d\xi</math> holds for almost every {{mvar|x}}.  As a result, the Fourier transform is [[injective]] on [[Lp space|{{math|''L''<sup>1</sup>('''R''')}}]].

=== Plancherel theorem and Parseval's theorem ===
{{main|Plancherel theorem|Parseval's theorem}}
Let {{tmath|f(x)}} and {{tmath|g(x)}} be integrable, and let {{tmath|\widehat{f}|(\xi)}} and {{tmath|\widehat{g}|(\xi)}} be their Fourier transforms. If {{tmath|f(x)}} and {{tmath|g(x)}} are also [[square-integrable]], then the Parseval formula follows:<ref>{{harvnb|Rudin|1987|p=187}}</ref>
<math display="block">\langle f, g\rangle_{L^{2}} = \int_{-\infty}^{\infty} f(x) \overline{g(x)} \,dx = \int_{-\infty}^\infty \widehat{f}(\xi) \overline{\widehat{g}(\xi)} \,d\xi,</math>
where the bar denotes [[complex conjugation]].

The [[Plancherel theorem]], which follows from the above, states that<ref>{{harvnb|Rudin|1987|p=186}}</ref>
<math display="block">\|f\|^2_{L^{2}} = \int_{-\infty}^\infty \left| f(x) \right|^2\,dx = \int_{-\infty}^\infty \left| \widehat{f}(\xi) \right|^2\,d\xi. </math>

Plancherel's theorem makes it possible to extend the Fourier transform, by a continuity argument, to a [[unitary operator]] on {{tmath|L^2(\R)}}. On {{tmath|L^1(\R) \cap L^2(\R)}}, this extension agrees with original Fourier transform defined on {{tmath|L^1(\R)}}, thus enlarging the domain of the Fourier transform to {{tmath|L^1(\R) + L^2(\R)}} (and consequently to {{tmath|L^p(\R)}} for {{tmath|1 \le p \le 2}}). Plancherel's theorem has the interpretation in the sciences that the Fourier transform preserves the [[energy]] of the original quantity. The terminology of these formulas is not quite standardised. [[Parseval's theorem]] was proved only for Fourier series, and was first proved by Lyapunov. But Parseval's formula makes sense for the Fourier transform as well, and so even though in the context of the Fourier transform it was proved by Plancherel, it is still often referred to as Parseval's formula, or Parseval's relation, or even Parseval's theorem.

See ''[[Pontryagin duality]]'' for a general formulation of this concept in the context of locally compact abelian groups.

=== Convolution theorem ===
{{main|Convolution theorem}}

The Fourier transform translates between [[convolution]] and multiplication of functions. If {{tmath|f(x)}} and {{tmath|g(x)}} are integrable functions with Fourier transforms {{tmath|\widehat{f}|(\xi)}} and {{tmath|\widehat{g}(\xi)}} respectively, then the Fourier transform of the convolution is given by the product of the Fourier transforms {{tmath|\widehat{f}|(\xi)}} and {{tmath|\widehat{g}|(\xi)}} (under other conventions for the definition of the Fourier transform a constant factor may appear).

This means that if:
<math display="block">h(x) = (f*g)(x) = \int_{-\infty}^\infty f(y)g(x - y)\,dy,</math>
where {{math|∗}} denotes the convolution operation, then:
<math display="block">\widehat{h}(\xi) = \widehat{f}(\xi)\, \widehat{g}(\xi).</math>

In [[LTI system theory|linear time invariant (LTI) system theory]], it is common to interpret {{tmath|g(x)}} as the [[impulse response]] of an LTI system with input {{tmath|f(x)}} and output {{tmath|h(x)}}, since substituting the [[Dirac delta function|unit impulse]] for {{tmath|f(x)}} yields {{tmath|1=h(x) = g(x)}}. In this case, {{tmath|\widehat{g}(\xi)}} represents the [[frequency response]] of the system.

Conversely, if {{tmath|f(x)}} can be decomposed as the product of two square integrable functions {{tmath|p(x)}} and {{tmath|q(x)}}, then the Fourier transform of {{tmath|f(x)}} is given by the convolution of the respective Fourier transforms {{tmath|\widehat{p}(\xi)}} and {{tmath|\widehat{q}(\xi)}}.

=== Cross-correlation theorem ===
{{main|Cross-correlation|Wiener–Khinchin theorem}}

In an analogous manner, it can be shown that if {{tmath|h(x)}} is the [[cross-correlation]] of {{tmath|f(x)}} and {{tmath|g(x)}}:
<math display="block">h(x) = (f \star g)(x) = \int_{-\infty}^\infty \overline{f(y)}g(x + y)\,dy</math>
then the Fourier transform of {{tmath|h(x)}} is:
<math display="block">\widehat{h}(\xi) = \overline{\widehat{f}(\xi)} \, \widehat{g}(\xi).</math>

As a special case, the [[autocorrelation]] of function {{tmath|f(x)}} is:
<math display="block">h(x) = (f \star f)(x) = \int_{-\infty}^\infty \overline{f(y)}f(x + y)\,dy</math>
for which
<math display="block">\widehat{h}(\xi) = \overline{\widehat{f}(\xi)}\widehat{f}(\xi) = \left|\widehat{f}(\xi)\right|^2.</math>

=== Differentiation ===
Suppose {{math|''f''(''x'')}} is differentiable [[almost everywhere]], and both {{tmath|f}} and its derivative {{tmath|f'}} are integrable (in {{tmath| L^1(\mathbb R) }}). Then the Fourier transform of the derivative is given by
<math display="block">\widehat{f'}(\xi) = \mathcal{F}\left\{ \frac{d}{dx} f(x)\right\} = i 2\pi \xi\widehat{f}(\xi).</math>
More generally, the Fourier transformation of the {{tmath|n}}th derivative {{tmath| f^{(n)} }} is given by
<math display="block">\widehat{f^{(n)}}(\xi) = \mathcal{F}\left\{ \frac{d^n}{dx^n} f(x) \right\} = (i 2\pi \xi)^n\widehat{f}(\xi).</math>

Analogously, {{tmath|1= \mathcal{F}^{-1}\left\{ \frac{d^n}{d\xi^n} \widehat{f}(\xi)\right\} = (-i 2\pi x)^n f(x) }}, so {{tmath|1= \mathcal{F}\left\{ x^n f(x)\right\} = \left(\frac{i}{2\pi}\right)^n \frac{d^n}{d\xi^n} \widehat{f}(\xi) }}.

By applying the Fourier transform and using these formulas, some [[ordinary differential equation]]s can be transformed into algebraic equations, which are much easier to solve. These formulas also give rise to the [[rule of thumb]] "{{tmath|f(x)}} is smooth [[if and only if]] {{tmath|\widehat{f}(\xi)}} quickly falls to {{tmath|0}} for {{tmath|\vert \xi \vert \to \infty }}". By using the analogous rules for the inverse Fourier transform, one can also say "{{tmath|f(x)}} quickly falls to {{tmath| 0 }} for {{tmath| \vert x \vert \to \infty}} if and only if {{tmath|\widehat{f}(\xi)}} is smooth."

=== Eigenfunctions ===
{{see also|Mehler kernel|Hermite polynomials#Hermite functions as eigenfunctions of the Fourier transform}}
The Fourier transform is a linear transform that has [[eigenfunction]]s obeying {{tmath|1= \mathcal{F}[\psi] = \lambda \psi }}, with {{tmath| \lambda \in \C }}.

A set of eigenfunctions is found by noting that the homogeneous differential equation 
<math display="block">\left[ U\left( \frac{1}{2\pi}\frac{d}{dx} \right) + U( x ) \right] \psi(x) = 0</math> 
leads to eigenfunctions <math>\psi(x)</math> of the Fourier transform <math>\mathcal{F}</math> as long as the form of the equation remains invariant under Fourier transform.{{refn|group=note|The operator <math display="inline">U\left( \frac{1}{2\pi}\frac{d}{dx} \right)</math> is defined by replacing <math>x</math> by <math display="inline">\frac{1}{2\pi}\frac{d}{dx}</math> in the [[Taylor series|Taylor expansion]] of {{tmath| U(x) }}.}} In other words, every solution <math>\psi(x)</math> and its Fourier transform <math>\widehat\psi(\xi)</math> obey the same equation. Assuming [[Ordinary differential equation#Existence and uniqueness of solutions|uniqueness]] of the solutions, every solution <math>\psi(x)</math> must therefore be an eigenfunction of the Fourier transform. The form of the equation remains unchanged under Fourier transform if <math>U(x)</math> can be expanded in a power series in which for all terms the same factor of either one of {{tmath| \pm 1 }}, {{tmath| \pm i}} arises from the factors <math>i^n</math> introduced by the [[#Differentiation|differentiation]] rules upon Fourier transforming the homogeneous differential equation because this factor may then be cancelled. The simplest allowable <math>U(x)=x</math> leads to the [[Normal distribution#Fourier transform and characteristic function|standard normal distribution]].<ref>{{harvnb|Folland|1992|p=216}}</ref>

More generally, a set of eigenfunctions is also found by noting that the [[#Differentiation|differentiation]] rules imply that the [[ordinary differential equation]] 
<math display="block">\left[ W\left( \frac{i}{2\pi}\frac{d}{dx} \right) + W(x) \right] \psi(x) = C \psi(x)</math>
with <math>C</math> constant and <math>W(x)</math> being a non-constant even function remains invariant in form when applying the Fourier transform <math>\mathcal{F}</math> to both sides of the equation. The simplest example is provided by {{tmath|1= W(x) = x^2}}, which is equivalent to considering the Schrödinger equation for the [[Quantum harmonic oscillator#Natural length and energy scales|quantum harmonic oscillator]].<ref>{{harvnb|Wolf|1979|p=307ff}}</ref> The corresponding solutions provide an important choice of an orthonormal basis for [[Square-integrable function|{{math|''L''<sup>2</sup>('''R''')}}]] and are given by the "physicist's" [[Hermite polynomials#Hermite functions as eigenfunctions of the Fourier transform|Hermite functions]]. Equivalently one may use
<math display="block">\psi_n(x) = \frac{\sqrt[4]{2}}{\sqrt{n!}} e^{-\pi x^2}\mathrm{He}_n\left(2x\sqrt{\pi}\right),</math>
where {{tmath| \mathrm{He}_n(x) }} are the "probabilist's" [[Hermite polynomial]]s, defined as
<math display="block">\mathrm{He}_n(x) = (-1)^n e^{\frac{1}{2}x^2}\left(\frac{d}{dx}\right)^n e^{-\frac{1}{2}x^2}.</math>

Under this convention for the Fourier transform, we have that
<math display="block">\widehat\psi_n(\xi) = (-i)^n \psi_n(\xi).</math>

In other words, the Hermite functions form a complete [[orthonormal]] system of [[eigenfunctions]] for the Fourier transform on {{tmath|L^2(\R)}}.<ref name="Pinsky-2002" /><ref>{{harvnb|Folland|1989|p=53}}</ref> However, this choice of eigenfunctions is not unique. Because of <math>\mathcal{F}^4 = \mathrm{id}</math> there are only four different [[eigenvalue]]s of the Fourier transform (the fourth roots of unity {{tmath|\pm 1}} and {{tmath|\pm i}}) and any linear combination of eigenfunctions with the same eigenvalue gives another eigenfunction.<ref>{{harvnb|Celeghini|Gadella|del Olmo|2021}}</ref> As a consequence of this, it is possible to decompose {{math|''L''<sup>2</sup>('''R''')}} as a direct sum of four spaces {{math|''H''<sub>0</sub>}}, {{math|''H''<sub>1</sub>}}, {{math|''H''<sub>2</sub>}}, and {{math|''H''<sub>3</sub>}} where the Fourier transform acts on {{math|H<sub>''k''</sub>}} simply by multiplication by {{math|''i''<sup>''k''</sup>}}.

Since the complete set of Hermite functions {{math|''ψ<sub>n</sub>''}} provides a resolution of the identity they diagonalize the Fourier operator, i.e. the Fourier transform can be represented by such a sum of terms weighted by the above eigenvalues, and these sums can be explicitly summed:
<math display="block">\mathcal{F}[f](\xi) = \int dx f(x) \sum_{n \geq 0} (-i)^n \psi_n(x) \psi_n(\xi) ~.</math>

This approach to define the Fourier transform was first proposed by [[Norbert Wiener]].<ref name="Duoandikoetxea-2001">{{harvnb|Duoandikoetxea|2001}}</ref> Among other properties, Hermite functions decrease exponentially fast in both frequency and time domains, and they are thus used to define a generalization of the Fourier transform, namely the [[fractional Fourier transform]] used in time–frequency analysis.<ref name="Boashash-2003">{{harvnb|Boashash|2003}}</ref> In [[physics]], this transform was introduced by [[Edward Condon]].<ref>{{harvnb|Condon|1937}}</ref> This [[change of basis]] becomes possible because the Fourier transform is a unitary transform when using the right [[#Other conventions|conventions]]. Consequently, under the proper conditions it may be expected to result from a self-adjoint generator <math>N</math> via<ref>{{harvnb|Wolf|1979|p=320}}</ref>
<math display="block">\mathcal{F}[\psi] = e^{-i t N} \psi.</math>

The operator <math>N</math> is the [[Quantum harmonic oscillator#Ladder operator method|number operator]] of the quantum harmonic oscillator written as<ref name="auto">{{harvnb|Wolf|1979|p=312}}</ref><ref>{{harvnb|Folland|1989|p=52}}</ref>
<math display="block">N \equiv \frac{1}{4\pi}\left(2\pi x - \frac{\partial}{\partial x}\right)\left(2\pi x + \frac{\partial}{\partial x}\right) = -\frac{1}{4\pi}\frac{\partial^2}{\partial x^2} + \pi x^2 - \frac{1}{2}.</math>

It can be interpreted as the [[symmetry in quantum mechanics|generator]] of [[Mehler kernel#Fractional Fourier transform|fractional Fourier transforms]] for arbitrary values of {{mvar|t}}, and of the conventional continuous Fourier transform <math>\mathcal{F}</math> for the particular value {{tmath|1= t = \pi/2 }}, with the [[Mehler kernel#Physics version|Mehler kernel]] implementing the corresponding [[active and passive transformation#In abstract vector spaces|active transform]]. The eigenfunctions of <math>N</math> are the [[Hermite polynomials#Hermite functions|Hermite functions]] {{tmath| \psi_n(x) }}, which are therefore also eigenfunctions of {{tmath| \mathcal{F} }}.

Upon extending the Fourier transform to [[distribution (mathematics)|distributions]] the [[Dirac comb#Fourier transform|Dirac comb]] is also an eigenfunction of the Fourier transform.

=== Inversion and periodicity ===
{{further|Fourier inversion theorem|Fractional Fourier transform}}

Under suitable conditions on the function {{tmath| f }}, it can be recovered from its Fourier transform {{tmath| \widehat{f} }}. Indeed, denoting the Fourier transform operator by {{tmath| \mathcal{F} }}, so {{tmath|1= \mathcal{F} f := \widehat{f} }}, then for suitable functions, applying the Fourier transform twice simply flips the function: {{tmath|1= \left(\mathcal{F}^2 f\right)(x) = f(-x) }}, which can be interpreted as "reversing time". Since reversing time is two-periodic, applying this twice yields {{tmath|1= \mathcal{F}^4(f) = f }}, so the Fourier transform operator is four-periodic, and similarly the inverse Fourier transform can be obtained by applying the Fourier transform three times: {{tmath|1= \mathcal{F}^3\left(\widehat{f}\right) = f }}. In particular the Fourier transform is invertible (under suitable conditions).

More precisely, defining the ''parity operator'' <math>\mathcal{P}</math> such that {{tmath|1= (\mathcal{P} f)(x) = f(-x) }}, we have:
<math display="block">\begin{align}
  \mathcal{F}^0 &= \mathrm{id}, \\
  \mathcal{F}^1 &= \mathcal{F}, \\
  \mathcal{F}^2 &= \mathcal{P}, \\
  \mathcal{F}^3 &= \mathcal{F}^{-1} = \mathcal{P} \circ \mathcal{F} = \mathcal{F} \circ \mathcal{P}, \\
  \mathcal{F}^4 &= \mathrm{id}
\end{align}</math>
These equalities of operators require careful definition of the space of functions in question, defining equality of functions (equality at every point? equality [[almost everywhere]]?) and defining equality of operators – that is, defining the topology on the function space and operator space in question. These are not true for all functions, but are true under various conditions, which are the content of the various forms of the [[Fourier inversion theorem]].

This fourfold periodicity of the Fourier transform is similar to a rotation of the plane by 90°, particularly as the two-fold iteration yields a reversal, and in fact this analogy can be made precise. While the Fourier transform can simply be interpreted as switching the time domain and the frequency domain, with the inverse Fourier transform switching them back, more geometrically it can be interpreted as a rotation by 90° in the [[time–frequency domain]] (considering time as the {{tmath|x}}-axis and frequency as the {{tmath|y}}-axis), and the Fourier transform can be generalized to the [[fractional Fourier transform]], which involves rotations by other angles. This can be further generalized to [[linear canonical transformation]]s, which can be visualized as the action of the [[special linear group]] [[SL2(R)|{{math|SL<sub>2</sub>('''R''')}}]] on the time–frequency plane, with the preserved symplectic form corresponding to the [[#Uncertainty principle|uncertainty principle]], below. This approach is particularly studied in [[signal processing]], under [[time–frequency analysis]].

=== Connection with the Heisenberg group ===
The [[Heisenberg group]] is a certain [[group (mathematics)|group]] of [[unitary operator]]s on the [[Hilbert space]] {{math|''L''<sup>2</sup>('''R''')}} of square integrable complex valued functions {{mvar|f}} on the real line, generated by the translations {{math|1=(''T<sub>y</sub> f'')(''x'') = ''f'' (''x'' + ''y'')}} and multiplication by {{math|''e''<sup>''i''2π''ξx''</sup>}}, {{math|1=(''M<sub>ξ</sub> f'')(''x'') = ''e''<sup>''i''2π''ξx''</sup> ''f'' (''x'')}}. These operators do not commute, as their (group) commutator is
<math display="block">\left(M^{-1}_\xi T^{-1}_y M_\xi T_yf\right)(x) = e^{i 2\pi\xi y}f(x) ,</math>
which is multiplication by the constant (independent of {{mvar|x}}) {{math|''e''<sup>''i''2π''ξy''</sup> ∈ ''U''(1)}} (the [[circle group]] of unit modulus complex numbers). As an abstract group, the Heisenberg group is the three-dimensional [[Lie group]] of triples {{math|(''x'', ''ξ'', ''z'') ∈ '''R'''<sup>2</sup> × ''U''(1)}}, with the group law
<math display="block">\left(x_1, \xi_1, t_1\right) \cdot \left(x_2, \xi_2, t_2\right) = \left(x_1 + x_2, \xi_1 + \xi_2, t_1 t_2 e^{-2 i \pi x_1 \xi_2}\right).</math>

Denote the Heisenberg group by {{math|''H''<sub>1</sub>}}. The above procedure describes not only the group structure, but also a standard [[unitary representation]] of {{math|''H''<sub>1</sub>}} on a Hilbert space, which we denote by {{math|''ρ'' : ''H''<sub>1</sub> → ''B''(''L''<sup>2</sup>('''R'''))}}. Define the linear automorphism of {{math|'''R'''<sup>2</sup>}} by
<math display="block">J \begin{pmatrix}
   x \\
  \xi
\end{pmatrix} = \begin{pmatrix}
  -\xi \\
    x
\end{pmatrix}</math>
so that {{math|1=''J''{{isup|2}} = −''I''}}. This {{mvar|J}} can be extended to a unique automorphism of {{math|''H''<sub>1</sub>}}:
<math display="block">j\left(x, \xi, t\right) = \left(-\xi, x, te^{-i 2\pi\xi x}\right).</math>

According to the [[Stone–von Neumann theorem]], the unitary representations {{mvar|ρ}} and {{math|''ρ'' ∘ ''j''}} are unitarily equivalent, so there is a unique intertwiner {{math|''W'' ∈ ''U''(''L''<sup>2</sup>('''R'''))}} such that
<math display="block">\rho \circ j = W \rho W^*.</math>
This operator {{mvar|W}} is the Fourier transform.

Many of the standard properties of the Fourier transform are immediate consequences of this more general framework.<ref>{{harvnb|Howe|1980}}</ref> For example, the square of the Fourier transform, {{math|''W''{{isup|2}}}}, is an intertwiner associated with {{math|1=''J''{{isup|2}} = −''I''}}, and so we have {{math|1=(''W''{{i sup|2}}''f'')(''x'') = ''f'' (−''x'')}} is the reflection of the original function {{mvar|f}}.

== Complex domain ==
The [[integral]] for the Fourier transform
<math display="block"> \widehat f (\xi) = \int _{-\infty}^\infty e^{-2i \pi t \xi} f(t) \, dt </math>
can be studied for [[complex number|complex]] values of its argument {{mvar|ξ}}. Depending on the properties of {{mvar|f}}, this might not converge off the real axis at all, or it might converge to a [[complex analysis|complex]] [[analytic function]] for all values of {{math|''ξ'' {{=}} ''σ'' + ''iτ''}}, or something in between.<ref>{{harvnb|Paley|Wiener|1934}}</ref>

The [[Paley–Wiener theorem]] says that {{mvar|f}} is smooth (i.e., {{mvar|n}}-times differentiable for all positive integers {{mvar|n}}) and compactly supported if and only if {{math|''f̂'' (''σ'' + ''iτ'')}} is a [[holomorphic function]] for which there exists a [[constant (mathematics)|constant]] {{math|''a'' > 0}} such that for any [[integer]] {{math|''n'' ≥ 0}},
<math display="block"> \left\vert \xi ^n \widehat f(\xi) \right\vert \leq C_n e^{2\pi a\vert\tau\vert} </math>
for some constant {{mvar|C_n}}. (In this case, {{mvar|f}} is supported on {{math|[−''a'', ''a'']}}.) This can be expressed by saying that {{math|''f̂''}} is an [[entire function]] that is [[rapidly decreasing]] in {{mvar|σ}} (for fixed {{mvar|τ}}) and of exponential growth in {{mvar|τ}} (uniformly in {{mvar|σ}}).<ref>{{harvnb|Gelfand|Vilenkin|1964}}</ref>

(If {{mvar|f}} is not smooth, but only {{math|''L''<sup>2</sup>}}, a corresponding version holds with the rapid-decrease condition replaced by the appropriate {{math|''L''<sup>2</sup>}} condition.<ref>{{harvnb|Kirillov|Gvishiani|1982}}</ref>) The space of such functions of a [[complex analysis|complex variable]] is called the Paley–Wiener space. This theorem has been generalised to semisimple [[Lie group]]s.<ref>{{harvnb|Clozel|Delorme|1985|pp=331–333}}</ref>

If {{mvar|f}} is supported on the half-line {{math|''t'' ≥ 0}}, then {{mvar|f}} is said to be "causal" because the [[impulse response function]] of a physically realisable [[Filter (mathematics)|filter]] must have this property, as no effect can precede its cause. [[Raymond Paley|Paley]] and Wiener showed that then, under suitable integrability hypotheses, {{math|''f̂''}} extends to a [[holomorphic function]] on the complex lower half-plane {{math|''τ'' < 0}} that tends to zero as {{mvar|τ}} goes to {{math|−∞}}.<ref>{{harvnb|de Groot|Mazur|1984|p=146}}</ref> A simple converse in this form is false; precise converses require additional growth or Hardy-space hypotheses.<ref>{{harvnb|Champeney|1987|p=80}}</ref>

=== Laplace transform ===
{{see also|Laplace transform#Fourier transform}}
The Fourier transform {{math|''f̂''(''ξ'')}} is related to the [[Laplace transform]] {{math|''F''(''s'')}}, which is also used for the solution of [[differential equation]]s and the analysis of [[Filter (signal processing)|filter]]s.

It may happen that a function {{mvar|f}} for which the Fourier integral does not converge on the real axis at all nevertheless has a complex Fourier transform defined in some region of the [[complex plane]].

For example, if {{mvar|f}} is causal and of exponential growth, i.e.,
<math display="block"> f(t)=0\quad (t<0), \qquad \vert f(t) \vert < C e^{at}\quad (t\geq 0) </math>
for some constants {{math|''C'', ''a'' ≥ 0}}, then<ref name="Kolmogorov-Fomin-1999">{{harvnb|Kolmogorov|Fomin|1999}}</ref>
<math display="block"> \widehat f (i\tau) = \int _0^\infty e^{ 2\pi \tau t} f(t) \, dt, </math>
convergent for all {{math|2π''τ'' < −''a''}}, is a one-sided Laplace transform of {{mvar|f}}.

The usual one-sided version of the Laplace transform is
<math display="block"> F(s) = \int_0^\infty f(t) e^{-st} \, dt.</math>

If {{mvar|f}} is causal and the integrals converge, then {{tmath|1= \widehat f(i\tau) = F(-2\pi\tau) }}. Thus, extending the Fourier transform to the complex domain means it includes the Laplace transform as a special case in the case of causal functions—but with the change of variable {{math|''s'' {{=}} ''i''2π''ξ''}}.

From another, perhaps more classical viewpoint, the Laplace transform by its form involves an additional exponential regulating term that lets it converge outside of the imaginary line where the Fourier transform is defined. As such it can converge for functions and integrals with at most exponential growth in the regulated direction, whereas the original Fourier decomposition cannot, enabling analysis of systems with divergent or critical elements. Two particular examples from linear signal processing are the construction of allpass filter networks from critical comb and mitigating filters via exact pole-zero cancellation on the unit circle. Such designs are common in audio processing, where highly nonlinear [[phase response]] is sought for, as in reverb.

Furthermore, when extended pulselike impulse responses are sought for signal processing work, the easiest way to produce them is to have one circuit that produces a divergent time response, and then to cancel its divergence through a delayed opposite and compensatory response. There, only the delay circuit in-between admits a classical Fourier description, which is critical. Both the circuits to the side are unstable, and do not admit a convergent Fourier decomposition. However, they do admit a Laplace domain description, with compatible half-planes of convergence in the complex plane (or in the discrete case, the Z-plane), wherein their effects cancel.

In modern mathematics the Laplace transform is conventionally subsumed under the aegis of Fourier methods. Both of them are subsumed by the far more general, and more abstract, idea of [[harmonic analysis]].

=== Inversion ===
Still with {{tmath|1= \xi = \sigma+ i\tau }}, if <math>\widehat f</math> is complex analytic for {{math|''a'' ≤ ''τ'' ≤ ''b''}} and has sufficient decay in horizontal strips, then
<math display="block"> \int _{-\infty}^\infty \widehat f (\sigma + ia) e^{ i 2\pi (\sigma+ia) t} \, d\sigma = \int _{-\infty}^\infty \widehat f (\sigma + ib) e^{ i 2\pi (\sigma+ib) t} \, d\sigma </math>
by [[Cauchy's integral theorem]]. Therefore, the Fourier inversion formula can use integration along different lines, parallel to the real axis.<ref>{{harvnb|Wiener|1949}}</ref>

Theorem: If {{math|1=''f''(''t'') = 0}} for {{math|''t'' < 0}}, and {{math|{{abs|''f''(''t'')}} < ''Ce''<sup>''at''</sup>}} for some constants {{math|''C'', ''a'' > 0}} and {{math|''t'' ≥ 0}}, then
<math display="block"> f(t) = \int_{-\infty}^\infty \widehat f(\sigma + i\tau) e^{i 2 \pi (\sigma+i\tau) t} \, d\sigma,</math>
for any {{math|''τ'' < −{{sfrac|''a''|2π}}}}, under the usual hypotheses for Fourier inversion.

This theorem implies the [[inverse Laplace transform#Mellin's inverse formula|Mellin inversion formula]] for the Laplace transformation,<ref name="Kolmogorov-Fomin-1999" />
<math display="block"> f(t) = \frac 1 {i 2\pi} \int_{b-i\infty}^{b+i\infty} F(s) e^{st}\, ds</math>
for any {{math|''b'' > ''a''}}, where {{math|''F''(''s'')}} is the Laplace transform of {{math|''f''(''t'')}}.

The hypotheses can be weakened, as in standard Fourier inversion results, to {{math|''f''(''t'') ''e''<sup>−''at''</sup>}} being {{math|''L''<sup>1</sup>}}, provided that {{mvar|f}} be of [[bounded variation]] in a closed neighborhood of {{mvar|t}} (cf. [[Dini test]]), the value of {{mvar|f}} at {{mvar|t}} be taken to be the [[arithmetic mean]] of the left and right limits, and that the integrals be taken in the sense of Cauchy principal values.<ref>{{harvnb|Champeney|1987|p=63}}</ref>

{{math|''L''<sup>2</sup>}} versions of these inversion formulas are also available.<ref>{{harvnb|Widder|Wiener|1938|p=537}}</ref>

== Fourier transform on Euclidean space ==
The Fourier transform can be defined in any arbitrary number of dimensions {{mvar|n}}. As with the one-dimensional case, there are many conventions. For an integrable function {{math|''f''('''x''')}}, this article takes the definition:
<math display="block">\widehat{f}(\boldsymbol{\xi}) = \mathcal{F}(f)(\boldsymbol{\xi}) = \int_{\R^n} f(\mathbf{x}) e^{-i 2\pi \boldsymbol{\xi}\cdot\mathbf{x}} \, d\mathbf{x}</math>
where {{math|'''x'''}} and {{math|'''ξ'''}} are {{mvar|n}}-dimensional [[vector (mathematics)|vectors]], and {{math|'''x''' · '''ξ'''}} is the [[dot product]] of the vectors. Alternatively, {{math|'''ξ'''}} can be viewed as belonging to the [[dual space|dual vector space]] {{tmath| \R^{n\star} }}, in which case the dot product becomes the [[tensor contraction|contraction]] of {{math|'''x'''}} and {{math|'''ξ'''}}, usually written as {{math|{{angbr|'''x''', '''ξ'''}}}}.

All of the basic properties listed above hold for the {{mvar|n}}-dimensional Fourier transform, as do Plancherel's and Parseval's theorem. When the function is integrable, the Fourier transform is still uniformly continuous and the [[Riemann–Lebesgue lemma]] holds.<ref name="Stein-Weiss-1971" />

=== Uncertainty principle ===
{{further|Uncertainty principle}}

Generally speaking, the more concentrated {{math|''f''(''x'')}} is, the more spread out its Fourier transform {{math|''f̂''(''ξ'')}} must be. In particular, the scaling property of the Fourier transform may be seen as saying: if we squeeze a function in {{mvar|x}}, its Fourier transform stretches out in {{mvar|ξ}}. It is not possible to arbitrarily concentrate both a function and its Fourier transform.

The trade-off between the compaction of a function and its Fourier transform can be formalized in the form of an [[uncertainty principle]] by viewing a function and its Fourier transform as [[conjugate variables]] with respect to the [[symplectic vector space|symplectic form]] on the [[time–frequency representation|time–frequency domain]]: from the point of view of the [[linear canonical transformation]], the Fourier transform is rotation by 90° in the time–frequency domain, and preserves the symplectic form.

Suppose {{math|''f''(''x'')}} is an integrable and [[square-integrable]] function. [[Without loss of generality]], assume that {{math|''f''(''x'')}} is normalized:
<math display="block">\int_{-\infty}^\infty |f(x)|^2 \,dx=1.</math>

It follows from the [[Plancherel theorem]] that {{math|''f̂''(''ξ'')}} is also normalized.

The spread around {{math|''x'' {{=}} 0}} may be measured by the ''dispersion about zero'' defined by<ref>{{harvnb|Pinsky|2002|loc=chpt. 2.4.3 The Uncertainty Principle}}</ref>
<math display="block">D_0(f)=\int_{-\infty}^\infty x^2|f(x)|^2\,dx.</math>

In probability terms, this is the [[Moment (mathematics)|second moment]] of {{math|{{abs|''f''(''x'')}}<sup>2</sup>}} about zero.

The uncertainty principle states that, if {{math|''f''(''x'')}} is absolutely continuous and the functions {{math|''x''·''f''(''x'')}} and {{math|''f''{{′}}(''x'')}} are square integrable, then
<math display="block">D_0(f)D_0(\widehat{f}) \geq \frac{1}{16\pi^2}.</math>

The equality is attained only in the case
<math display="block">\begin{align} f(x) &= C_1 \, e^{-\pi \frac{x^2}{\sigma^2} }\\
\therefore \widehat{f}(\xi) &= \sigma C_1 \, e^{-\pi\sigma^2\xi^2} \end{align} </math>
where {{math|''σ'' > 0}} is arbitrary and {{math|1=''C''<sub>1</sub> = {{sfrac|{{radic|2|4}}|{{sqrt|''σ''}}}}}} so that {{mvar|f}} is {{math|''L''<sup>2</sup>}}-normalized. In other words, where {{mvar|f}} is a (normalized) [[Gaussian function]] with variance {{math|''σ''<sup>2</sup>/2{{pi}}}}, centered at zero, and its Fourier transform is a Gaussian function with variance {{math|''σ''<sup>−2</sup>/2{{pi}}}}.  Gaussian functions are examples of [[Schwartz function]]s (see the discussion on tempered distributions below).

In fact, this inequality implies that:
<math display="block">\left(\int_{-\infty}^\infty (x-x_0)^2|f(x)|^2\,dx\right)\left(\int_{-\infty}^\infty(\xi-\xi_0)^2\left|\widehat{f}(\xi)\right|^2\,d\xi\right)\geq \frac{1}{16\pi^2}, \quad \forall x_0, \xi_0 \in \mathbb{R}.</math>
In [[quantum mechanics]], the [[momentum]] and position [[wave function]]s are Fourier transform pairs, up to a factor of the [[Planck constant]]. With this constant properly taken into account, the inequality above becomes the statement of the [[Heisenberg uncertainty principle]].<ref>{{harvnb|Stein|Shakarchi|2003|loc= chpt. 5.4 The Heisenberg uncertainty principle}}</ref>

A stronger uncertainty principle is the [[Hirschman uncertainty|Hirschman uncertainty principle]], which is expressed as:
<math display="block">H\left(\left|f\right|^2\right)+H\left(\left|\widehat{f}\right|^2\right)\ge \log\left(\frac{e}{2}\right)</math>
where {{math|''H''(''p'')}} is the [[differential entropy]] of the [[probability density function]] {{math|''p''(''x'')}}:
<math display="block">H(p) = -\int_{-\infty}^\infty p(x)\log\bigl(p(x)\bigr) \, dx</math>
where the logarithms may be in any base that is consistent. The equality is attained for a Gaussian, as in the previous case.

=== Sine and cosine transforms ===
{{main|Sine and cosine transforms}}

Fourier's original formulation of the transform did not use complex numbers, but rather sines and cosines. Statisticians and others still use this form. An absolutely integrable function {{mvar|f}} for which Fourier inversion holds can be expanded in terms of genuine frequencies (avoiding negative frequencies, which are sometimes considered hard to interpret physically<ref>{{harvnb|Chatfield|2004|p=113}}</ref>) {{mvar|λ}} by
<math display="block">f(t) = \int_0^\infty \bigl( a(\lambda ) \cos( 2\pi \lambda t) + b(\lambda ) \sin( 2\pi \lambda t)\bigr) \, d\lambda.</math>

This is called an expansion as a [[trigonometric integral]], or a Fourier integral expansion. The coefficient functions {{mvar|a}} and {{mvar|b}} can be found by using variants of the Fourier cosine transform and the Fourier sine transform (the normalisations are, again, not standardised):
<math display="block"> a (\lambda) = 2\int_{-\infty}^\infty f(t) \cos(2\pi\lambda t) \, dt</math>
and
<math display="block"> b (\lambda) = 2\int_{-\infty}^\infty f(t) \sin(2\pi\lambda t) \, dt. </math>

Older literature refers to the two transform functions, the Fourier cosine transform, {{mvar|a}}, and the Fourier sine transform, {{mvar|b}}.

The function {{mvar|f}} can be recovered from the sine and cosine transform using
<math display="block"> f(t) = 2\int_0 ^{\infty} \int_{-\infty}^{\infty} f(\tau) \cos\bigl( 2\pi \lambda(\tau-t)\bigr) \, d\tau \, d\lambda.</math>
together with trigonometric identities. This is referred to as Fourier's integral formula.<ref name="Kolmogorov-Fomin-1999" /><ref>{{harvnb|Fourier|1822|p=441}}</ref><ref>{{harvnb|Poincaré|1895|p=102}}</ref><ref>{{harvnb|Whittaker|Watson|1927|p=188}}</ref>

=== Spherical harmonics ===
Let the set of [[Homogeneous polynomial|homogeneous]] [[Harmonic function|harmonic]] [[polynomial]]s of degree {{mvar|k}} on {{math|'''R'''<sup>''n''</sup>}} be denoted by {{math|'''A'''<sub>''k''</sub>}}. The set {{math|'''A'''<sub>''k''</sub>}} consists of the [[solid spherical harmonics]] of degree {{mvar|k}}. The solid spherical harmonics play a similar role in higher dimensions to the Hermite polynomials in dimension one. Specifically, if {{math|1=''f''(''x'') = ''e''<sup>−π{{abs|''x''}}<sup>2</sup></sup>''P''(''x'')}} for some {{math|''P''(''x'')}} in {{math|'''A'''<sub>''k''</sub>}}, then {{tmath|1= \widehat{f}(\xi) = i^{-k} f(\xi) }}. Let the set {{math|'''H'''<sub>''k''</sub>}} be the closure in {{math|''L''<sup>2</sup>('''R'''<sup>''n''</sup>)}} of linear combinations of functions of the form {{math|''f''({{abs|''x''}})''P''(''x'')}} where {{math|''P''(''x'')}} is in {{math|'''A'''<sub>''k''</sub>}}. The space {{math|''L''<sup>2</sup>('''R'''<sup>''n''</sup>)}} is then a direct sum of the spaces {{math|'''H'''<sub>''k''</sub>}} and the Fourier transform maps each space {{math|'''H'''<sub>''k''</sub>}} to itself and it is possible to characterize the action of the Fourier transform on each space {{math|'''H'''<sub>''k''</sub>}}.<ref name="Stein-Weiss-1971" />

Let {{math|1=''f''(''x'') = ''f''<sub>0</sub>({{abs|''x''}})''P''(''x'')}} (with {{math|''P''(''x'')}} in {{math|'''A'''<sub>''k''</sub>}}), then
<math display="block">\widehat{f}(\xi)=F_0(|\xi|)P(\xi)</math>
where
<math display="block">F_0(r) = 2\pi i^{-k}r^{-\frac{n+2k-2}{2}} \int_0^\infty f_0(s)J_\frac{n+2k-2}{2}(2\pi rs)s^\frac{n+2k}{2}\,ds.</math>

Here {{math|''J''<sub>(''n'' + 2''k'' − 2)/2</sub>}} denotes the [[Bessel function]] of the first kind with order {{math|{{sfrac|''n'' + 2''k'' − 2|2}}}}. When {{math|''k'' {{=}} 0}} this gives a useful formula for the Fourier transform of a radial function.<ref>{{harvnb|Grafakos|2004}}</ref> This is essentially the [[Hankel transform]]. Moreover, there is a simple recursion relating the cases {{math|''n'' + 2}} and {{mvar|n}}<ref>{{harvnb|Grafakos|Teschl|2013}}</ref> allowing to compute, e.g., the three-dimensional Fourier transform of a radial function from the one-dimensional one.

=== Restriction problems ===
{{see also|Fourier extension operator}}
In higher dimensions it becomes interesting to study ''restriction problems'' for the Fourier transform. The Fourier transform of an integrable function is continuous and the restriction of this function to any set is defined. But for a square-integrable function the Fourier transform could be a general ''class'' of square integrable functions. As such, the restriction of the Fourier transform of an {{math|''L''<sup>2</sup>('''R'''<sup>''n''</sup>)}} function cannot be defined on sets of measure 0. It is still an active area of study to understand restriction problems in {{math|''L''{{isup|''p''}}}} for {{math|1 < ''p'' < 2}}. It is possible in some cases to define the restriction of a Fourier transform to a set {{mvar|S}}, provided {{mvar|S}} has non-zero curvature. The case when {{mvar|S}} is the unit sphere in {{math|'''R'''<sup>''n''</sup>}} is of particular interest. In this case the Tomas–[[Elias Stein|Stein]] restriction theorem states that the restriction of the Fourier transform to the unit sphere in {{math|'''R'''<sup>''n''</sup>}} is a bounded operator on {{math|''L''{{isup|''p''}}}} provided {{math|1 ≤ ''p'' ≤ {{sfrac|2''n'' + 2|''n'' + 3}}}}.

One notable difference between the Fourier transform in 1 dimension versus higher dimensions concerns the partial sum operator. Consider an increasing collection of measurable sets {{math|''E''<sub>''R''</sub>}} indexed by {{math|''R'' ∈ (0, ∞)}}: such as balls of radius {{mvar|R}} centered at the origin, or cubes of side {{math|2''R''}}. For a given integrable function {{mvar|f}}, consider the function {{mvar|f<sub>R</sub>}} defined by:
<math display="block">f_R(x) = \int_{E_R}\widehat{f}(\xi) e^{i 2\pi x\cdot\xi}\, d\xi, \quad x \in \mathbb{R}^n.</math>

Suppose in addition that {{math|''f'' ∈ ''L''{{isup|''p''}}('''R'''<sup>''n''</sup>)}}. For {{math|''n'' {{=}} 1}} and {{math|1 < ''p'' < ∞}}, if one takes {{math|''E<sub>R</sub>'' {{=}} (−''R'', ''R'')}}, then {{mvar|f<sub>R</sub>}} converges to {{mvar|f}} in {{math|''L''{{isup|''p''}}}} as {{mvar|R}} tends to infinity, by the boundedness of the [[Hilbert transform]]. Naively one may hope the same holds true for {{math|''n'' > 1}}. In the case that {{mvar|E<sub>R</sub>}} is taken to be a cube with side length {{mvar|R}}, then convergence still holds. Another natural candidate is the Euclidean ball {{math|''E''<sub>''R''</sub> {{=}} {''ξ'' : {{abs|''ξ''}} < ''R''{{)}}}}. In order for this partial sum operator to converge, it is necessary that the [[Multiplier (Fourier analysis)|multiplier]] for the unit ball be bounded in {{math|''L''{{isup|''p''}}('''R'''<sup>''n''</sup>)}}. For {{math|''n'' ≥ 2}} it is a celebrated theorem of [[Charles Fefferman]] that the multiplier for the unit ball is never bounded unless {{math|''p'' {{=}} 2}}.<ref>{{harvnb|Duoandikoetxea|2001|loc=Thm. 8.3}}</ref> In fact, when {{math|''p'' ≠ 2}}, this shows that not only may {{mvar|f<sub>R</sub>}} fail to converge to {{mvar|f}} in {{math|''L''{{isup|''p''}}}}, but for some functions {{math|''f'' ∈ ''L''{{isup|''p''}}('''R'''<sup>''n''</sup>)}}, {{mvar|f<sub>R</sub>}} is not even an element of {{math|''L''{{isup|''p''}}}}.

== Fourier transform on function spaces ==
{{see also|Riesz–Thorin theorem}}
The definition of the Fourier transform naturally extends from <math>L^1(\mathbb R)</math> to {{tmath| L^1(\mathbb R^n) }}. That is, if <math>f \in L^1(\mathbb{R}^n)</math> then the Fourier transform 
<math>\mathcal{F}:L^1(\mathbb{R}^n) \to L^\infty(\mathbb{R}^n)</math> is given by <math display="block">f(x)\mapsto \widehat{f}(\xi) = \int_{\mathbb{R}^n} f(x)e^{-i 2\pi \xi\cdot x}\,dx, \quad \forall \xi \in \mathbb{R}^n.</math>
This operator is [[bounded operator|bounded]] as
<math display="block">\sup_{\xi \in \mathbb{R}^n}\left\vert\widehat{f}(\xi)\right\vert \leq \int_{\mathbb{R}^n} \vert f(x)\vert \,dx,</math>
which shows that its [[operator norm]] is bounded by {{math|1}}. The [[Riemann–Lebesgue lemma]] shows that if <math>f\in L^1(\mathbb{R}^n)</math> then its Fourier transform actually belongs to the [[Function space#Functional analysis|space of continuous functions that vanish at infinity]], i.e., {{tmath| \widehat{f} \in C_{0}(\mathbb{R}^n)\subset L^{\infty}(\mathbb{R}^n) }}.{{sfn|ps=|Stein|Weiss|1971|pp=1–2}}{{sfn|ps=|Rudin|1987|pp=182–183}} Furthermore, the [[Image (mathematics)|image]] of <math>L^1</math> under <math>\mathcal{F}</math> is a strict subset of {{tmath| C_{0}(\mathbb{R}^n) }}.{{sfn|ps=|Chandrasekharan|1989|pp=7–8,84}}
 
Similarly to the case of one variable, the Fourier transform can be defined on {{tmath| L^2(\mathbb R^n) }}. The Fourier transform in <math>L^2(\mathbb R^n)</math> is no longer given by an ordinary Lebesgue integral, although it can be computed by an [[improper integral]], i.e.,
<math display="block">\widehat{f}(\xi) = \lim_{R\to\infty}\int_{|x|\le R} f(x) e^{-i 2\pi\xi\cdot x}\,dx</math>
where the limit is taken in the {{math|''L''<sup>2</sup>}} sense.{{refn|group=note|More generally, one can take a sequence of functions that are in the intersection of {{math|''L''<sup>1</sup>}} and {{math|''L''<sup>2</sup>}} and that converges to {{mvar|f}} in the {{math|''L''<sup>2</sup>}}-norm, and define the Fourier transform of {{mvar|f}} as the {{math|''L''<sup>2</sup>}} -limit of the Fourier transforms of these functions.}}<ref>{{cite web |url=https://statweb.stanford.edu/~candes/teaching/math262/Lectures/Lecture03.pdf |title=Applied Fourier Analysis and Elements of Modern Signal Processing Lecture 3 |date= January 12, 2016|access-date=2019-10-11|archive-url=https://web.archive.org/web/20201003042302/https://statweb.stanford.edu/~candes/teaching/math262/Lectures/Lecture03.pdf |archive-date=2020-10-03 }}</ref>

Furthermore, <math>\mathcal{F}:L^2(\mathbb{R}^n) \to L^2(\mathbb{R}^n)</math> is a [[unitary operator]].{{sfn|ps=|Stein|Weiss|1971|loc=Thm. 2.3}} For an operator to be unitary it is sufficient to show that it is bijective and preserves the inner product. The Fourier inversion theorem implies that the transform is bijective. Also, for any {{math|''f'', ''g'' ∈ ''L''<sup>2</sup>('''R'''<sup>''n''</sup>)}} we have
<math display="block">\int_{\mathbb{R}^n} f(x)\mathcal{F}g(x)\,dx = \int_{\mathbb{R}^n} \mathcal{F}f(x)g(x)\,dx. </math>
So
<math display="block">
\begin{align}
\int_{\mathbb{R}^n} \overline{\mathcal{F}f(x)}\mathcal{F}g(x)\,dx
 &= \int_{\mathbb{R}^n} \mathcal{F}^{-1}\overline{f(x)}\mathcal{F}g(x)\,dx\\
 &= \int_{\mathbb{R}^n} \mathcal{F}\mathcal{F}^{-1}\overline{f(x)}g(x)\,dx
 = \int_{\mathbb{R}^n} \overline{f(x)}g(x)\,dx
\end{align}
</math>

So the transform preserves the inner product.

=== On other ''L''<sup>''p''</sup> ===
For {{tmath| 1<p<2 }}, the Fourier transform can be defined on <math>L^p(\mathbb R)</math> by [[Riesz–Thorin interpolation]], which amounts to decomposing such functions into a fat tail part <math>|f|\le 1</math> in {{math|''L''<sup>2</sup>}} plus a fat body part <math>|f|>1</math> in {{math|''L''<sup>1</sup>}}. In each of these spaces, the Fourier transform of a function in {{math|''L''{{isup|''p''}}('''R'''<sup>''n''</sup>)}} is in {{math|''L''{{isup|''q''}}('''R'''<sup>''n''</sup>)}}, where {{math|1=''q'' = {{sfrac|''p''|''p'' − 1}}}} is the [[Hölder conjugate]] of {{mvar|p}} (by the [[Hausdorff–Young inequality]]). However, except for {{math|1=''p'' = 2}}, the image is not easily characterized. Further extensions become more technical. The Fourier transform of functions in {{math|''L''{{isup|''p''}}}} for the range {{math|2 < ''p'' < ∞}} requires the study of distributions.{{sfn|ps=|Katznelson|2004}} In fact, it can be shown that there are functions in {{math|''L''{{isup|''p''}}}} with {{math|''p'' > 2}} so that the Fourier transform is not defined as a function.<ref name="Stein-Weiss-1971" />

=== Tempered distributions ===
{{main|Distribution (mathematics)#Tempered distributions and Fourier transform}}
{{see also|Rigged Hilbert space}}
One might consider enlarging the domain of the Fourier transform from <math>L^1 + L^2</math> by considering [[generalized function]]s, or distributions. A distribution on <math>\mathbb{R}^n</math> is a continuous linear functional on the space <math>C_c^\infty(\mathbb{R}^n)</math> of compactly supported smooth functions (i.e. [[bump function]]s), equipped with a suitable topology.  Since <math>C_c^\infty(\mathbb{R}^n)</math> is dense in {{tmath| L^{2}(\mathbb{R}^n) }}, the [[Plancherel theorem]] allows one to extend the definition of the Fourier transform to general functions in <math>L^2(\mathbb{R}^n)</math> by continuity arguments. The strategy is then to consider the action of the Fourier transform on <math>C_c^\infty(\mathbb{R}^n)</math> and pass to distributions by duality. The obstruction to doing this is that the Fourier transform does not map <math>C_c^\infty(\mathbb{R}^n)</math> to {{tmath| C_c^\infty(\mathbb{R}^n) }}. In fact the Fourier transform of an element in <math>C_c^\infty(\mathbb{R}^n)</math> can not vanish on an open set; see the above discussion on the uncertainty principle.{{sfn|ps=|Mallat|2009|p=45}}{{sfn|ps=|Strichartz|1994|p=150}}

The Fourier transform can also be defined for [[tempered distribution]]s {{tmath| \mathcal S'(\mathbb R^n) }}, dual to the space of [[Schwartz function]]s {{tmath| \mathcal S(\mathbb R^n) }}. A Schwartz function is a smooth function that decays at infinity, along with all of its derivatives, hence <math>C_c^\infty(\mathbb{R}^n)\subset  \mathcal S(\mathbb R^n)</math> and:
<math display="block">\mathcal{F}: C_c^\infty(\mathbb{R}^n) \rightarrow \mathcal S(\mathbb R^n) \setminus  C_c^\infty(\mathbb{R}^n).</math> The Fourier transform is an [[automorphism]] of the Schwartz space and, by duality, also an automorphism of the space of tempered distributions.<ref name="Stein-Weiss-1971" />{{sfn|ps=|Hunter|2014}} The tempered distributions include well-behaved functions of polynomial growth, distributions of compact support as well as all the integrable functions mentioned above.

For the definition of the Fourier transform of a tempered distribution, let <math>f</math> and <math>g</math> be integrable functions, and let <math>\widehat{f}</math> and <math>\widehat{g}</math> be their Fourier transforms respectively. Then the Fourier transform obeys the following multiplication formula,<ref name="Stein-Weiss-1971" />
<math display="block">\int_{\mathbb{R}^n}\widehat{f}(x)g(x)\,dx=\int_{\mathbb{R}^n}f(x)\widehat{g}(x)\,dx.</math>

Every integrable function <math>f</math> defines (induces) a distribution <math>T_f</math> by the relation
<math display="block">T_f(\varphi)=\int_{\mathbb{R}^n}f(x)\varphi(x)\,dx,\quad \forall \varphi\in\mathcal S(\mathbb R^n).</math>
So it makes sense to define the Fourier transform of a tempered distribution <math>T_{f}\in\mathcal S'(\mathbb R)</math> by the duality:
<math display="block">\langle \widehat T_f, \varphi\rangle = \langle T_f,\widehat \varphi\rangle,\quad \forall \varphi\in\mathcal S(\mathbb R^n).</math>
Extending this to all tempered distributions <math>T</math> gives the general definition of the Fourier transform.

Distributions can be differentiated and the above-mentioned compatibility of the Fourier transform with differentiation and convolution remains true for tempered distributions.

== Generalizations ==

=== Fourier–Stieltjes transform on measurable spaces <span class="anchor" id="Fourier-Stieltjes transform"></span> ===
{{see also|Bochner–Minlos theorem|Riesz–Markov–Kakutani representation theorem|Fourier series#Fourier-Stieltjes series}}
The Fourier transform of a [[finite measure|finite]] [[Borel measure]] {{mvar|μ}} on {{math|'''R'''<sup>''n''</sup>}}, given by the bounded, uniformly continuous function:{{sfn|ps=|Pinsky|2002|p=256}}{{sfn|ps=|Rudin|1991|p=15}}
<math display="block">\widehat\mu(\xi)=\int_{\mathbb{R}^n} e^{-i 2\pi x \cdot \xi}\,d\mu,</math>
is called the ''Fourier–Stieltjes transform'' due to its connection with the [[Riemann–Stieltjes integral#Application to functional analysis|Riemann-Stieltjes integral]] representation of [[Radon measure|(Radon) measures]].{{sfn|ps=|Edwards|1982|pp=53,67,72–73}} If <math>\mu</math> is the [[probability distribution]] of a [[random variable]] <math>X</math> then its Fourier–Stieltjes transform is, by definition, a [[Characteristic function (probability theory)|characteristic function]].<ref>{{harvnb|Katznelson|2004|p=173}} {{pb}} The typical conventions in probability theory take {{math|''e''<sup>''iξx''</sup>}} instead of {{math|''e''<sup>−''i''2π''ξx''</sup>}}.</ref> If, in addition, the probability distribution has a [[probability density function]], this definition is subject to the usual Fourier transform.{{sfn|ps=|Billingsley|1995|p=345}} Stated more generally, when <math>\mu</math> is [[Absolute continuity#Absolute continuity of measures|absolutely continuous]] with respect to the Lebesgue measure, i.e., 
<math display="block"> d\mu = f(x) \, dx,</math>
then
<math display="block">\widehat{\mu}(\xi)=\widehat{f}(\xi),</math>
and the Fourier-Stieltjes transform reduces to the usual definition of the Fourier transform. That is, the notable difference with the Fourier transform of integrable functions is that the Fourier-Stieltjes transform need not vanish at infinity, i.e., the [[Riemann–Lebesgue lemma]] fails for measures.{{sfn|ps=|Katznelson|2004|pp=40,155,164}}

[[Bochner's theorem]] characterizes which functions may arise as the Fourier–Stieltjes transform of a positive measure on the circle.

One example of a finite Borel measure that is not a function is the [[Dirac measure]].{{sfn|ps=|Edwards|1982|p=53}} Its Fourier transform is a constant function (whose value depends on the form of the Fourier transform used).

=== Locally compact abelian groups ===
{{main|Pontryagin duality}}
The Fourier transform may be generalized to any [[locally compact abelian group]], i.e., an [[abelian group]] that is also a [[locally compact Hausdorff space]] such that the group operation is continuous. If {{mvar|G}} is a locally compact abelian group, it has a translation invariant measure {{mvar|μ}}, called [[Haar measure]]. For a locally compact abelian group {{mvar|G}}, the set of irreducible, i.e. one-dimensional, unitary representations are called its [[character group|characters]]. With its natural group structure and the topology of uniform convergence on compact sets (that is, the topology induced by the [[compact-open topology]] on the space of all continuous functions from <math>G</math> to the [[circle group]]), the set of characters {{mvar|Ĝ}} is itself a locally compact abelian group, called the ''Pontryagin dual'' of {{mvar|G}}. For a function {{mvar|f}} in {{math|''L''<sup>1</sup>(''G'')}}, its Fourier transform is defined by{{sfn|ps=|Katznelson|2004}}
<math display="block">\widehat{f}(\xi) = \int_G \overline{\xi(x)}f(x)\,d\mu\quad \text{for any }\xi \in \widehat{G}.</math>

The Riemann–Lebesgue lemma holds in this case; {{math|''f̂''(''ξ'')}} is a function vanishing at infinity on {{mvar|Ĝ}}.

The Fourier transform on {{nowrap|{{mvar|T}} {{=}} R/Z}} is an example; here {{mvar|T}} is a locally compact abelian group, and the Haar measure {{mvar|μ}} on {{mvar|T}} can be thought of as the Lebesgue measure on [0,1). Consider a representation of {{mvar|T}} on the complex plane {{mvar|C}} thought of as a 1-dimensional complex vector space. There is a group of such representations (which are irreducible since {{mvar|C}} is 1-dim) <math>\{e_{k}: T \rightarrow GL_{1}(C) = C^{*} \mid k \in Z\}</math> where <math>e_{k}(x) = e^{i 2\pi kx}</math> for {{tmath| x\in T }}.

The character of such representation, that is the trace of <math>e_{k}(x)</math> (thought of as a one-by-one matrix) for each <math>x\in T</math> and {{tmath| k\in Z }}, is <math>e^{i 2\pi kx}</math> itself. Now, in the case of representations of finite groups, the character table of a group {{mvar|G}} consists of rows of vectors such that each row is the character of one irreducible representation of {{mvar|G}}, and these vectors form an orthonormal basis of the space of class (meaning conjugation-invariant) functions that map from {{mvar|G}} to {{mvar|C}} by Schur's lemma. The group {{mvar|T}} is no longer finite but still compact, and it preserves the orthonormality of the character table. Each row of the table is the function <math>e_{k}(x)</math> of {{tmath| x\in T }}, and the inner product between two class functions (all functions being class functions since {{mvar|T}} is abelian) <math>f,g \in L^{2}(T, d\mu)</math> is defined as <math display="inline">\langle f, g \rangle = \frac{1}{|T|}\int_{[0,1)}f(y)\overline{g}(y)d\mu(y)</math> with the normalizing factor {{tmath|1= \vert T \vert = 1 }}. The sequence <math>\{e_{k}\mid k\in Z\}</math> is an orthonormal basis of the space of class functions {{tmath| L^{2}(T,d\mu) }}.

For any representation {{mvar|V}} of a finite group {{mvar|G}}, <math>\chi_{v}</math> can be expressed as the span <math display="inline">\sum_{i} \left\langle \chi_{v},\chi_{v_{i}} \right\rangle \chi_{v_{i}}</math> (<math>V_{i}</math> are the irreducible representations of {{mvar|G}}), such that {{tmath|1= \textstyle \left\langle \chi_{v}, \chi_{v_{i} } \right\rangle = \frac{1}{\vert G \vert}\sum_{g\in G}\chi_{v}(g)\overline{\chi}_{v_{i} }(g) }}. Similarly for <math>G = T</math> and {{tmath| f\in L^{2}(T, d\mu) }}, {{tmath|1= \textstyle f(x) = \sum_{k\in Z}\widehat{f}(k)e_{k} }}. The Pontriagin dual <math>\widehat{T}</math> is <math>\{e_{k}\}(k\in Z)</math> and for {{tmath| f \in L^{2}(T, d\mu) }}, <math display="inline">\widehat{f}(k) = \frac{1}{|T|}\int_{[0,1)}f(y)e^{-i 2\pi ky}dy</math> is its Fourier transform for {{tmath| e_{k} \in \widehat{T} }}.

=== Gelfand transform ===
{{main|Gelfand representation}}
The Fourier transform is also a special case of the [[Gelfand transform]]. In this particular context, it is closely related to the Pontryagin duality map defined above.

Given an abelian [[locally compact space|locally compact]] [[Hausdorff space|Hausdorff]] [[topological group]] {{mvar|G}}, as before we consider the space {{math|''L''<sup>1</sup>(''G'')}}, defined using a Haar measure. With convolution as multiplication, {{math|''L''<sup>1</sup>(''G'')}} is an abelian [[Banach algebra]]. It also has an [[Involution (mathematics)|involution]] * given by
<math display="block">f^*(g) = \overline{f\left(g^{-1}\right)}.</math>

Taking the completion with respect to the largest possible {{math|''C''*}}-norm gives its enveloping {{math|''C''*}}-algebra, called the group {{math|''C''*}}-algebra {{math|''C''*(''G'')}} of {{mvar|G}}. (Any {{math|''C''*}}-norm on {{math|''L''<sup>1</sup>(''G'')}} is bounded by the {{math|''L''<sup>1</sup>}} norm, therefore their supremum exists.)

Given any abelian {{math|''C''*}}-algebra {{mvar|A}}, the Gelfand transform gives an isomorphism between {{mvar|A}} and {{math|''C''<sub>0</sub>(''A''^)}}, where {{math|''A''^}} is the multiplicative linear functionals, i.e. one-dimensional representations, on {{mvar|A}} with the weak-* topology. The map is simply given by
<math display="block">a \mapsto \bigl( \varphi \mapsto \varphi(a) \bigr).</math>
It turns out that the multiplicative linear functionals of {{math|''C''*(''G'')}}, after suitable identification, are exactly the characters of {{mvar|G}}, and the Gelfand transform, when restricted to the dense subset {{math|''L''<sup>1</sup>(''G'')}}, is the Fourier–Pontryagin transform.

=== Compact non-abelian groups ===
The Fourier transform can also be defined for functions on a non-abelian group, provided that the group is [[compact space|compact]]. Removing the assumption that the underlying group is abelian, irreducible unitary representations need not always be one-dimensional. This means the Fourier transform on a non-abelian group takes values as Hilbert space operators.<ref>{{harvnb|Hewitt|Ross|1970|loc=Chapter 8}}</ref> The Fourier transform on compact groups is a major tool in [[representation theory]]<ref>{{harvnb|Knapp|2001}}</ref> and [[non-commutative harmonic analysis]].

Let {{mvar|G}} be a compact [[Hausdorff space|Hausdorff]] [[topological group]], and let {{mvar|λ}} be its normalized [[Haar measure]]. Let {{math|Σ}} denote the collection of all isomorphism classes of finite-dimensional irreducible [[unitary representation]]s, along with a definite choice of representation {{math|''U''{{isup|(''σ'')}}}} on the [[Hilbert space]] {{math|''H<sub>σ</sub>''}} of finite dimension {{math|''d<sub>σ</sub>''}} for each {{math|''σ'' ∈ Σ}}.

For {{math|''f'' ∈ ''L''<sup>1</sup>(''G'')}}, the Fourier transform of {{mvar|f}} at {{math|σ}} is the operator on {{math|''H<sub>σ</sub>''}} defined by
<math display="block">
\widehat f(\sigma)=\int_G f(g) U^{(\sigma)}_{g^{-1}}\,d\lambda(g).
</math>
Equivalently,
<math display="block">
\left\langle \widehat f(\sigma)\xi,\eta\right\rangle_{H_\sigma}
=
\int_G f(g)\left\langle U^{(\sigma)}_{g^{-1}}\xi,\eta\right\rangle\,d\lambda(g).
</math>
Since {{math|''U''{{isup|(''σ'')}}}} is unitary, this may also be written using the adjoint <math>{U^{(\sigma)}}_g^*</math>.

If {{mvar|μ}} is a finite complex [[Borel measure]] on {{mvar|G}}, then the Fourier–Stieltjes transform of {{mvar|μ}} is the operator on {{math|''H<sub>σ</sub>''}} defined by
<math display="block">
\widehat\mu(\sigma)=\int_G U^{(\sigma)}_{g^{-1}}\,d\mu(g),
</math>
or, weakly,
<math display="block">
\left\langle \widehat{\mu}(\sigma)\xi,\eta\right\rangle_{H_\sigma}
=
\int_G \left\langle U^{(\sigma)}_{g^{-1}}\xi,\eta\right\rangle\,d\mu(g).
</math>
If {{mvar|μ}} is [[absolutely continuous]] with respect to {{mvar|λ}}, [[Radon–Nikodym theorem|represented]] as
<math display="block">d\mu = f\,d\lambda</math>
for some {{math|''f'' ∈ [[Lp space|''L''<sup>1</sup>(''G'')]]}}, one identifies the Fourier transform of {{mvar|f}} with the Fourier–Stieltjes transform of {{mvar|μ}}.

The mapping
<math display="block">\mu\mapsto\widehat{\mu}</math>
is injective and sends finite measures to bounded fields of operators {{math|(\widehat\mu(\sigma))<sub>σ∈Σ</sub>}}, with
<math display="block">
\sup_{\sigma\in\Sigma}\|\widehat\mu(\sigma)\|\leq \|\mu\|.
</math>
Thus it may be viewed as a representation of the [[Banach algebra]] {{math|''M''(''G'')}} of finite Borel measures, with multiplication given by [[convolution]] of measures. With the convention above, convolution corresponds to operator multiplication with the order reversed:
<math display="block">
\widehat{\mu * \nu}(\sigma)=\widehat\nu(\sigma)\widehat\mu(\sigma).
</math>
Using the alternative convention {{math|1=\widehat f(\sigma)=\int_G f(g)U^{(\sigma)}_g\,d\lambda(g)}} reverses this order. The involution on {{math|''M''(''G'')}} is given, for absolutely continuous measures, by
<math display="block">
f^*(g)=\overline{f(g^{-1})},
</math>
since compact groups are unimodular.

The [[Peter–Weyl theorem]] holds, and a version of the Fourier inversion formula follows: if {{math|''f'' ∈ ''L''<sup>2</sup>(''G'')}}, then
<math display="block">
f(g)=\sum_{\sigma\in\Sigma} d_\sigma \operatorname{tr}\left(\widehat f(\sigma)U^{(\sigma)}_g\right),
</math>
where the summation is understood as convergent in the {{math|''L''<sup>2</sup>}} sense. The corresponding Plancherel formula is
<math display="block">
\|f\|_2^2
=
\sum_{\sigma\in\Sigma} d_\sigma \|\widehat f(\sigma)\|_{\mathrm{HS}}^2,
</math>
where {{math|{{!}}{{!}}·{{!}}{{!}}<sub>HS</sub>}} denotes the [[Hilbert–Schmidt operator|Hilbert–Schmidt norm]].

The generalization of the Fourier transform to the noncommutative situation has also in part contributed to the development of [[noncommutative geometry]].{{Citation needed|date=May 2009}} In this context, a categorical generalization of the Fourier transform to noncommutative groups is [[Tannaka–Krein duality]], which replaces the group of characters with the category of representations. However, this is no longer simply a transform of scalar-valued functions into scalar-valued functions.

== Alternatives ==
In [[signal processing]] terms, a function (of time) is a representation of a signal with perfect ''time resolution'', but no frequency information, while the Fourier transform has perfect ''frequency resolution'', but no time information: the magnitude of the Fourier transform at a point is how much frequency content there is, but location is only given by phase (argument of the Fourier transform at a point), and [[standing wave]]s are not localized in time – a sine wave continues out to infinity, without decaying. This limits the usefulness of the Fourier transform for analyzing signals that are localized in time, notably [[transient (acoustics)|transients]], or any signal of finite extent.

As alternatives to the Fourier transform, in [[time–frequency analysis]], one uses time–frequency transforms or time–frequency distributions to represent signals in a form that has some time information and some frequency information – by the uncertainty principle, there is a trade-off between these. These can be generalizations of the Fourier transform, such as the [[short-time Fourier transform]], [[fractional Fourier transform]], synchrosqueezing Fourier transform,{{sfn|ps=|Correia|Justo|Angélico|2024}} or other functions to represent signals, as in [[wavelet transform]]s and [[chirplet transform]]s, with the wavelet analog of the Fourier transform being the [[continuous wavelet transform]].<ref name="Boashash-2003" />

== Example ==
The following figures provide a visual illustration of how the Fourier transform's integral measures whether a frequency is present in a particular function. The first image depicts the function {{tmath|1= f(t) = \cos(2\pi\ 3 t) \ e^{-\pi t^2} }}, which is a 3&nbsp;[[hertz|Hz]] cosine wave (the first term) shaped by a [[Gaussian function|Gaussian]] [[Envelope (waves)|envelope function]] (the second term) that smoothly turns the wave on and off. The next 2 images show the product {{tmath| f(t) e^{-i 2\pi 3 t} }}, which must be integrated to calculate the Fourier transform at +3&nbsp;Hz. The real part of the integrand has a non-negative average value, because the alternating signs of <math>f(t)</math> and <math>\operatorname{Re}(e^{-i 2\pi 3 t})</math> oscillate at the same rate and in phase, whereas <math>f(t)</math> and <math>\operatorname{Im} (e^{-i 2\pi 3 t})</math> oscillate at the same rate but with orthogonal phase. The absolute value of the Fourier transform at +3&nbsp;Hz is 0.5, which is relatively large. When added to the Fourier transform at -3&nbsp;Hz (which is identical because we started with a real signal), we find that the amplitude of the 3&nbsp;Hz frequency component is 1.

[[File:Onfreq.png|class=skin-invert-image|left|thumb|695x695px|Original function, which has a strong 3&nbsp;Hz component. Real and imaginary parts of the integrand of its Fourier transform at +3&nbsp;Hz.]]
{{clear}}However, when you try to measure a frequency that is not present, both the real and imaginary component of the integral vary rapidly between positive and negative values. For instance, the red curve is looking for 5&nbsp;Hz. The absolute value of its integral is nearly zero, indicating that almost no 5&nbsp;Hz component was in the signal. The general situation is usually more complicated than this, but heuristically this is how the Fourier transform measures how much of an individual frequency is present in a function {{tmath| f(t) }}.<gallery widths="360px" heights="360px" class="skin-invert-image">
File:Offfreq i2p.svg| Real and imaginary parts of the integrand for its Fourier transform at +5&nbsp;Hz.
File:Fourier transform of oscillating function.svg| Magnitude of its Fourier transform, with +3 and +5&nbsp;Hz labeled.
</gallery>

To re-enforce an earlier point, the reason for the response at <math>\xi=-3</math> Hz is because <math>\cos(2\pi 3t)</math> and <math>\cos(2\pi(-3)t)</math> are indistinguishable.  The transform of &nbsp;<math>e^{i2\pi 3t}\cdot e^{-\pi t^2}</math>&nbsp; would have just one response, whose amplitude is the integral of the smooth envelope: {{tmath| e^{-\pi t^2} }}, whereas &nbsp;<math>\operatorname{Re}(f(t)\cdot e^{-i2\pi 3t})</math> is {{tmath| e^{-\pi t^2} (1 + \cos(2\pi 6t))/2 }}.

== Applications ==
{{see also|Spectral density#Applications}}

[[File:Commutative diagram illustrating problem solving via the Fourier transform.svg|class=skin-invert-image|thumb|400px|Some problems, such as certain differential equations, become easier to solve when the Fourier transform is applied. In that case the solution to the original problem is recovered using the inverse Fourier transform.]]

Linear operations performed in one domain (time or frequency) have corresponding operations in the other domain, which are sometimes easier to perform. The operation of [[derivative|differentiation]] in the time domain corresponds to multiplication by the frequency,{{refn|group=note|Up to an imaginary constant factor whose magnitude depends on what Fourier transform convention is used.}} so some [[differential equation]]s are easier to analyze in the frequency domain. Also, [[convolution]] in the time domain corresponds to ordinary multiplication in the frequency domain (see ''[[Convolution theorem]]''). After performing the desired operations, transformation of the result can be made back to the time domain. [[Harmonic analysis]] is the systematic study of the relationship between the frequency and time domains, including the kinds of functions or operations that are "simpler" in one or the other, and has deep connections to many areas of modern mathematics.

=== Analysis of differential equations ===
Perhaps the most important use of the Fourier transformation is to solve [[partial differential equation]]s.
Many of the equations of the mathematical physics of the nineteenth century can be treated this way. Fourier studied the heat equation, which in one dimension and in dimensionless units is
<math display="block">\frac{\partial^2 y(x, t)}{\partial^2 x} = \frac{\partial y(x, t)}{\partial t}.</math>
The example we will give, a slightly more difficult one, is the wave equation in one dimension,
<math display="block">\frac{\partial^2y(x, t)}{\partial^2 x} = \frac{\partial^2y(x, t)}{\partial^2t}.</math>

As usual, the problem is not to find a solution: there are infinitely many. The problem is that of the so-called "boundary problem": find a solution that satisfies the 'boundary conditions'
<math display="block">y(x, 0) = f(x),\qquad \frac{\partial y(x, 0)}{\partial t} = g(x).</math>

Here, {{mvar|f}} and {{mvar|g}} are given functions. For the heat equation, only one boundary condition can be required (usually the first one). But for the wave equation, there are still infinitely many solutions {{mvar|y}} that satisfy the first boundary condition. But when one imposes both conditions, there is only one possible solution.

It is easier to find the Fourier transform {{mvar|ŷ}} of the solution than to find the solution directly. This is because the Fourier transformation takes differentiation into multiplication by the Fourier-dual variable, and so a partial differential equation applied to the original function is transformed into multiplication by polynomial functions of the dual variables applied to the transformed function. After {{mvar|ŷ}} is determined, we can apply the inverse Fourier transformation to find {{mvar|y}}.

Fourier's method is as follows. First, note that any function of the forms
<math display="block"> \cos\bigl(2\pi\xi(x\pm t)\bigr) \text{ or } \sin\bigl(2\pi\xi(x \pm t)\bigr)</math>
satisfies the wave equation. These are called the elementary solutions.

Second, note that therefore any integral
<math display="block">\begin{align}
  y(x, t) = \int_{0}^{\infty} d\xi \Bigl[ &a_+(\xi)\cos\bigl(2\pi\xi(x + t)\bigr) + a_-(\xi)\cos\bigl(2\pi\xi(x - t)\bigr) +{} \\
                                     &b_+(\xi)\sin\bigl(2\pi\xi(x + t)\bigr) + b_-(\xi)\sin\left(2\pi\xi(x - t)\right) \Bigr]
\end{align}</math>
satisfies the wave equation for arbitrary {{math|''a''<sub>+</sub>, ''a''<sub>−</sub>, ''b''<sub>+</sub>, ''b''<sub>−</sub>}}. This integral may be interpreted as a continuous linear combination of solutions for the linear equation.

Now this resembles the formula for the Fourier synthesis of a function. In fact, this is the real inverse Fourier transform of {{math|''a''<sub>±</sub>}} and {{math|''b''<sub>±</sub>}} in the variable {{mvar|x}}.

The third step is to examine how to find the specific unknown coefficient functions {{math|''a''<sub>±</sub>}} and {{math|''b''<sub>±</sub>}} that will lead to {{mvar|y}} satisfying the boundary conditions. We are interested in the values of these solutions at {{math|1=''t'' = 0}}. So we will set {{math|1=''t'' = 0}}. Assuming that the conditions needed for Fourier inversion are satisfied, we can then find the Fourier sine and cosine transforms (in the variable {{mvar|x}}) of both sides and obtain
<math display="block"> 2\int_{-\infty}^\infty y(x,0) \cos(2\pi\xi x) \, dx = a_+ + a_-</math>
and
<math display="block">2\int_{-\infty}^\infty y(x,0) \sin(2\pi\xi x) \, dx = b_+ + b_-.</math>

Similarly, taking the derivative of {{mvar|y}} with respect to {{mvar|t}} and then applying the Fourier sine and cosine transformations yields
<math display="block">2\int_{-\infty}^\infty \frac{\partial y(u,0)}{\partial t} \sin (2\pi\xi x) \, dx = (2\pi\xi)\left(-a_+ + a_-\right)</math>
and
<math display="block">2\int_{-\infty}^\infty \frac{\partial y(u,0)}{\partial t} \cos (2\pi\xi x) \, dx = (2\pi\xi)\left(b_+ - b_-\right).</math>

These are four linear equations for the four unknowns {{math|''a''<sub>±</sub>}} and {{math|''b''<sub>±</sub>}}, in terms of the Fourier sine and cosine transforms of the boundary conditions, which are easily solved by elementary algebra, provided that these transforms can be found.

In summary, we chose a set of elementary solutions, parametrized by {{mvar|ξ}}, of which the general solution would be a (continuous) linear combination in the form of an integral over the parameter {{mvar|ξ}}. But this integral was in the form of a Fourier integral. The next step was to express the boundary conditions in terms of these integrals, and set them equal to the given functions {{mvar|f}} and {{mvar|g}}. But these expressions also took the form of a Fourier integral because of the properties of the Fourier transform of a derivative. The last step was to exploit Fourier inversion by applying the Fourier transformation to both sides, thus obtaining expressions for the coefficient functions {{math|''a''<sub>±</sub>}} and {{math|''b''<sub>±</sub>}} in terms of the given boundary conditions {{mvar|f}} and {{mvar|g}}.

From a higher point of view, Fourier's procedure can be reformulated more conceptually. Since there are two variables, we will use the Fourier transformation in both {{mvar|x}} and {{mvar|t}} rather than operate as Fourier did, who only transformed in the spatial variables. Note that {{mvar|ŷ}} must be considered in the sense of a distribution since {{math|''y''(''x'', ''t'')}} is not going to be {{math|''L''<sup>1</sup>}}: as a wave, it will persist through time and thus is not a transient phenomenon. But it will be bounded and so its Fourier transform can be defined as a distribution. The operational properties of the Fourier transformation that are relevant to this equation are that it takes differentiation in {{mvar|x}} to multiplication by {{math|''i''2π''ξ''}} and differentiation with respect to {{mvar|t}} to multiplication by {{math|''i''2π''f''}} where {{mvar|f}} is the frequency. Then the wave equation becomes an algebraic equation in {{mvar|ŷ}}:
<math display="block">\xi^2 \widehat y (\xi, f) = f^2 \widehat y (\xi, f).</math>
This is equivalent to requiring {{math|1=''ŷ''(''ξ'', ''f'') = 0}} unless {{math|1=''ξ'' = ±''f''}}. Right away, this explains why the choice of elementary solutions we made earlier worked so well: obviously {{math|1=''ŷ'' = ''δ''(''ξ'' ± ''f'')}} will be solutions. Applying Fourier inversion to these delta functions, we obtain the elementary solutions we picked earlier. But from the higher point of view, one does not pick elementary solutions, but rather considers the space of all distributions that are supported on the (degenerate) conic {{math|1=''ξ''{{isup|2}} − ''f''{{isup|2}} = 0}}.

We may as well consider the distributions supported on the conic that are given by distributions of one variable on the line {{math|1=''ξ'' = ''f''}} plus distributions on the line {{math|''ξ'' {{=}} −''f''}} as follows: if {{mvar|Φ}} is any test function,
<math display="block">\iint \widehat y \varphi(\xi,f) \, d\xi \, df = \int s_+ \varphi(\xi,\xi) \, d\xi + \int s_- \varphi(\xi,-\xi) \, d\xi,</math>
where {{math|''s''<sub>+</sub>}}, and {{math|''s''<sub>−</sub>}}, are distributions of one variable.

Then Fourier inversion gives, for the boundary conditions, something very similar to what we had more concretely above (put {{math|1=''Φ''(''ξ'', ''f'') = ''e''<sup>''i''2π(''xξ''+''tf'')</sup>}}, which is clearly of polynomial growth):
<math display="block"> y(x,0) = \int\bigl\{s_+(\xi) + s_-(\xi)\bigr\} e^{i 2\pi \xi x+0} \, d\xi </math>
and
<math display="block"> \frac{\partial y(x,0)}{\partial t} = \int\bigl\{s_+(\xi) - s_-(\xi)\bigr\} i 2\pi \xi e^{i 2\pi\xi x+0} \, d\xi.</math>

Now, as before, applying the one-variable Fourier transformation in the variable {{mvar|x}} to these functions of {{mvar|x}} yields two equations in the two unknown distributions {{math|''s''<sub>±</sub>}} (which can be taken to be ordinary functions if the boundary conditions are {{math|''L''<sup>1</sup>}} or {{math|''L''<sup>2</sup>}}).

From a calculational point of view, the drawback of course is that one must first calculate the Fourier transforms of the boundary conditions, then assemble the solution from these, and then calculate an inverse Fourier transform. Closed form formulas are rare, except when there is some geometric symmetry that can be exploited, and the numerical calculations are difficult because of the oscillatory nature of the integrals, which makes convergence slow and hard to estimate. For practical calculations, other methods are often used.

==== Nonlinear Fourier transform ====
{{main|Inverse scattering transform}}
The twentieth century has seen application of these methods to all linear partial differential equations with polynomial coefficients as well as an extension to certain classes of [[nonlinear partial differential equation]]s. Specifically, nonlinear evolution equations (i.e. those equations that describe how a particular quantity evolves in time from a specified initial state) that can be associated with linear eigenvalue problems whose eigenvalues are integrals of the nonlinear equations.{{sfn|ps=|Ablowitz|Kaup|Newell|Segur|1974|pp=249–315}}{{sfn|ps=|Lax|1968|pp=467–490}} As it may be considered an extension of Fourier analysis to nonlinear problems, the solution method is called the '''nonlinear Fourier transform''' (or '''[[inverse scattering transform]]''') method.{{sfn|ps=|Yousefi|Kschischang|2014|pp=4312–4328}}

=== Fourier-transform spectroscopy ===
{{main|Fourier-transform spectroscopy}}
The Fourier transform is also used in [[nuclear magnetic resonance]] (NMR) and in other kinds of [[spectroscopy]], e.g. infrared ([[Fourier-transform infrared spectroscopy|FTIR]]). In NMR an exponentially shaped free induction decay (FID) signal is acquired in the time domain and Fourier-transformed to a Lorentzian line-shape in the frequency domain. The Fourier transform is also used in [[magnetic resonance imaging]] (MRI) and [[mass spectrometry]].

=== Quantum mechanics ===
The Fourier transform is useful in [[quantum mechanics]] in at least two different ways. To begin with, the basic conceptual structure of quantum mechanics postulates the existence of pairs of [[complementary variables]], connected by the [[Heisenberg uncertainty principle]]. For example, in one dimension, the spatial variable {{mvar|q}} of, say, a particle, can only be measured by the quantum mechanical "[[position operator]]" at the cost of losing information about the momentum {{mvar|p}} of the particle. Therefore, the physical state of the particle can either be described by a function, called "the wave function", of {{mvar|q}} or by a function of {{mvar|p}} but not by a function of both variables. The variable {{mvar|p}} is called the conjugate variable to {{mvar|q}}.

In classical mechanics, the physical state of a particle (existing in one dimension, for simplicity of exposition) would be given by assigning definite values to both {{mvar|p}} and {{mvar|q}} simultaneously. Thus, the set of all possible physical states is the two-dimensional real vector space with a {{mvar|p}}-axis and a {{mvar|q}}-axis called the [[phase space]]. In contrast, quantum mechanics chooses a polarisation of this space in the sense that it picks a subspace of one-half the dimension, for example, the {{mvar|q}}-axis alone, but instead of considering only points, takes the set of all complex-valued "wave functions" on this axis. Nevertheless, choosing the {{mvar|p}}-axis is an equally valid polarisation, yielding a different representation of the set of possible physical states of the particle. Both representations of the wavefunction are related by a Fourier transform, such that 
<math display="block">\varphi(p) = \int dq\, \psi (q) e^{-i pq/h} ,</math>
or, equivalently, 
<math display="block">\psi(q) = \int dp \, \varphi (p) e^{i pq/h}.</math>

Physically realisable states are {{math|''L''<sup>2</sup>}}, and so by the [[Plancherel theorem]], their Fourier transforms are also {{math|''L''<sup>2</sup>}}.  (Note that since {{mvar|q}} is in units of distance and {{mvar|p}} is in units of momentum, the presence of the Planck constant in the exponent makes the exponent [[Nondimensionalization|dimensionless]], as it should be.)

Therefore, the Fourier transform can be used to pass from one way of representing the state of the particle, by a wave function of position, to another way of representing the state of the particle: by a wave function of momentum. Infinitely many different polarisations are possible, and all are equally valid. Being able to transform states from one representation to another by the Fourier transform is not only convenient but also the underlying reason of the Heisenberg [[#Uncertainty principle|uncertainty principle]].

The other use of the Fourier transform in both quantum mechanics and [[quantum field theory]] is to solve the applicable wave equation. In non-relativistic quantum mechanics, the [[Schrödinger equation]] for a time-varying wave function in one-dimension, not subject to external forces, is
<math display="block">-\frac{\partial^2}{\partial x^2} \psi(x,t) = i \frac h{2\pi} \frac{\partial}{\partial t} \psi(x,t).</math>

This is the same as the heat equation except for the presence of the imaginary unit {{mvar|i}}. Fourier methods can be used to solve this equation.

In the presence of a potential, given by the potential energy function {{math|''V''(''x'')}}, the equation becomes
<math display="block">-\frac{\partial^2}{\partial x^2} \psi(x,t) + V(x)\psi(x,t) = i \frac h{2\pi} \frac{\partial}{\partial t} \psi(x,t).</math>

The "elementary solutions", as we referred to them above, are the so-called "stationary states" of the particle, and Fourier's algorithm, as described above, can still be used to solve the boundary value problem of the future evolution of {{mvar|ψ}} given its values for {{math|''t'' {{=}} 0}}. Neither of these approaches is of much practical use in quantum mechanics. Boundary value problems and the time-evolution of the wave function is not of much practical interest: it is the stationary states that are most important.

In relativistic quantum mechanics, the Schrödinger equation becomes a wave equation as was usual in classical physics, except that complex-valued waves are considered. A simple example, in the absence of interactions with other particles or fields, is the free one-dimensional Klein–Gordon–Schrödinger–Fock equation, this time in dimensionless units,
<math display="block">\left (\frac{\partial^2}{\partial x^2} +1 \right) \psi(x,t) = \frac{\partial^2}{\partial t^2} \psi(x,t).</math>

This is, from the mathematical point of view, the same as the wave equation of classical physics solved above (but with a complex-valued wave, which makes no difference in the methods). This is of great use in quantum field theory: each separate Fourier component of a wave can be treated as a separate harmonic oscillator and then quantized, a procedure known as "second quantization". Fourier methods have been adapted to also deal with non-trivial interactions.

Finally, the [[Quantum harmonic oscillator#Ladder operator method|number operator]] of the [[quantum harmonic oscillator]] can be interpreted, for example via the [[Mehler kernel#Physics version|Mehler kernel]], as the [[Symmetry in quantum mechanics|generator]] of the [[#Eigenfunctions|Fourier transform]] {{tmath| \mathcal{F} }}.<ref name="auto"/>

=== Signal processing ===
The Fourier transform is used for the spectral analysis of time-series. The subject of statistical signal processing does not, however, usually apply the Fourier transformation to the signal itself. Even if a real signal is indeed transient, it has been found in practice advisable to model a signal by a function (or, alternatively, a stochastic process) that is stationary in the sense that its characteristic properties are constant over all time. The Fourier transform of such a function does not exist in the usual sense, and it has been found more useful for the analysis of signals to instead take the Fourier transform of its autocorrelation function.

The autocorrelation function {{mvar|R}} of a function {{mvar|f}} is defined by
<math display="block">R_f (\tau) = \lim_{T\rightarrow \infty} \frac{1}{2T} \int_{-T}^T f(t) f(t+\tau) \, dt. </math>

This function is a function of the time-lag {{mvar|τ}} elapsing between the values of {{mvar|f}} to be correlated.

For most functions {{mvar|f}} that occur in practice, {{mvar|R}} is a bounded even function of the time-lag {{mvar|τ}} and for typical noisy signals it turns out to be uniformly continuous with a maximum at {{math|''τ'' {{=}} 0}}.

The autocorrelation function, more properly called the autocovariance function unless it is normalized in some appropriate fashion, measures the strength of the correlation between the values of {{mvar|f}} separated by a time lag. This is a way of searching for the correlation of {{mvar|f}} with its own past. It is useful even for other statistical tasks besides the analysis of signals. For example, if {{math|''f''(''t'')}} represents the temperature at time {{mvar|t}}, one expects a strong correlation with the temperature at a time lag of 24 hours.

It possesses a Fourier transform,
<math display="block"> P_f(\xi) = \int_{-\infty}^\infty R_f (\tau) e^{-i 2\pi \xi\tau} \, d\tau. </math>

This Fourier transform is called the [[Spectral density#Power spectral density|power spectral density]] function of {{mvar|f}}. (Unless all periodic components are first filtered out from {{mvar|f}}, this integral will diverge, but it is easy to filter out such periodicities.)

The power spectrum, as indicated by this density function {{mvar|P}}, measures the amount of variance contributed to the data by the frequency {{mvar|ξ}}. In electrical signals, the variance is proportional to the average power (energy per unit time), and so the power spectrum describes how much the different frequencies contribute to the average power of the signal. This process is called the spectral analysis of time-series and is analogous to the usual analysis of variance of data that is not a time-series ([[ANOVA]]).

Knowledge of which frequencies are "important" in this sense is crucial for the proper design of filters and for the proper evaluation of measuring apparatuses. It can also be useful for the scientific analysis of the phenomena responsible for producing the data.

The power spectrum of a signal can also be approximately measured directly by measuring the average power that remains in a signal after all the frequencies outside a narrow band have been filtered out.

Spectral analysis is carried out for visual signals as well. The power spectrum ignores all phase relations, which is good enough for many purposes, but for video signals other types of spectral analysis must also be employed, still using the Fourier transform as a tool.

== Other notations ==
Other common notations for <math>\widehat f(\xi)</math> include:
<math display="block">\tilde{f}(\xi),\ F(\xi),\ \mathcal{F}\left(f\right)(\xi),\ \left(\mathcal{F}f\right)(\xi),\ \mathcal{F}(f),\ \mathcal{F}\{f\},\ \mathcal{F} \bigl(f(t)\bigr),\ \mathcal{F} \bigl\{f(t)\bigr\}.</math>

In the sciences and engineering it is also common to make substitutions like these:
<math display="block">\xi \rightarrow f, \quad x \rightarrow t, \quad f \rightarrow x,\quad \widehat f \rightarrow X.  </math>

So the transform pair <math>f(x)\ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ \widehat{f}(\xi)</math> can become <math>x(t)\ \stackrel{\mathcal{F}}{\Longleftrightarrow}\ X(f)</math>

A disadvantage of the capital letter notation is when expressing a transform such as <math>\widehat f\cdot g</math> or {{tmath| \widehat f' }}, which become the more awkward <math>\mathcal{F}\{f\cdot g\}</math> and {{tmath| \mathcal{F} \{ f' \} }}.

In some contexts such as particle physics, the same symbol <math>f</math> may be used for both for a function as well as it Fourier transform, with the two only distinguished by their [[Argument of a function|argument]]  I.e. <math>f(k_1 + k_2)</math> would refer to the Fourier transform because of the momentum argument, while <math>f(x_0 + \pi \vec r)</math> would refer to the original function because of the positional argument. Although tildes may be used as in <math>\tilde{f}</math> to indicate Fourier transforms, tildes may also be used to indicate a modification of a quantity with a more [[Lorentz invariant]] form, such as {{tmath|1= \tilde{dk} = \frac{dk}{(2\pi)^32\omega} }}, so care must be taken.  Similarly, <math>\widehat f</math> often denotes the [[Hilbert transform]] of {{tmath| f }}.

The interpretation of the complex function {{math|''f̂''(''ξ'')}} may be aided by expressing it in [[polar coordinate]] form
<math display="block">\widehat f(\xi) = A(\xi) e^{i\varphi(\xi)}</math>
in terms of the two real functions {{math|''A''(''ξ'')}} and {{math|''φ''(''ξ'')}} where:
<math display="block">A(\xi) = \left|\widehat f(\xi)\right|,</math>
is the [[amplitude]] and
<math display="block">\varphi (\xi) = \arg \left( \widehat f(\xi) \right), </math>
is the [[phase (waves)|phase]] (see ''[[Arg (mathematics)|Arg]]'').

Then the inverse transform can be written:
<math display="block">f(x) = \int _{-\infty}^\infty A(\xi)\ e^{ i\bigl(2\pi \xi x +\varphi (\xi)\bigr)}\,d\xi,</math>
which is a recombination of all the frequency components of {{math|''f''(''x'')}}. Each component is a complex [[sinusoid]] of the form {{math|''e''<sup>2π''ixξ''</sup>}} whose amplitude is {{math|''A''(''ξ'')}} and whose initial [[phase (waves)|phase angle]] (at {{math|1=''x'' = 0}}) is {{math|''φ''(''ξ'')}}.

The Fourier transform may be thought of as a mapping on function spaces. This mapping is here denoted {{mathcal|F}} and {{math|{{mathcal|F}}(''f'')}} is used to denote the Fourier transform of the function {{mvar|f}}. This mapping is linear, which means that {{mathcal|F}} can also be seen as a linear transformation on the function space and implies that the standard notation in linear algebra of applying a linear transformation to a vector (here the function {{math|''f''}}) can be used to write {{math|{{mathcal|F}} ''f''}} instead of {{math|{{mathcal|F}}(''f'')}}. Since the result of applying the Fourier transform is again a function, we can be interested in the value of this function evaluated at the value {{mvar|ξ}} for its variable, and this is denoted either as {{math|{{mathcal|F}} ''f''(''ξ'')}} or as {{math|({{mathcal|F}} ''f'')(''ξ'')}}. Notice that in the former case, it is implicitly understood that {{mathcal|F}} is applied first to {{mvar|f}} and then the resulting function is evaluated at {{mvar|ξ}}, not the other way around.

In mathematics and various applied sciences, it is often necessary to distinguish between a function {{mvar|f}} and the value of {{mvar|f}} when its variable equals {{mvar|x}}, denoted {{math|''f''(''x'')}}. This means that a notation like {{math|{{mathcal|F}}(''f''(''x''))}} formally can be interpreted as the Fourier transform of the values of {{mvar|f}} at {{mvar|x}}. Despite this flaw, the previous notation appears frequently, often when a particular function or a function of a particular variable is to be transformed. For example,
<math display="block">\mathcal F\bigl( \operatorname{rect}(x) \bigr) = \operatorname{sinc}(\xi)</math>
is sometimes used to express that the Fourier transform of a [[rectangular function]] is a [[sinc function]], or
<math display="block">\mathcal F\bigl(f(x + x_0)\bigr) = \mathcal F\bigl(f(x)\bigr)\, e^{i 2\pi x_0 \xi}</math>
is used to express the shift property of the Fourier transform.

Notice, that the last example is only correct under the assumption that the transformed function is a function of {{mvar|x}}, not of {{math|''x''<sub>0</sub>}}.

As discussed above, the [[Characteristic function (probability theory)|characteristic function]] of a random variable is the same as the [[#Fourier–Stieltjes transform|Fourier–Stieltjes transform]] of its distribution measure, but in this context it is typical to take a different convention for the constants. Typically characteristic function is defined
<math display="block">E\left(e^{it\cdot X}\right)=\int e^{it\cdot x} \, d\mu_X(x).</math>

As in the case of the "non-unitary angular frequency" convention above, the factor of 2{{pi}} appears in neither the normalizing constant nor the exponent. Unlike any of the conventions appearing above, this convention takes the opposite sign in the exponent.

== Computation methods ==
The appropriate computation method largely depends how the original mathematical function is represented and the desired form of the output function.  In this section we consider both functions of a continuous variable, {{tmath| f(x) }}, and functions of a discrete variable (i.e. ordered pairs of <math>x</math> and <math>f</math> values).  For discrete-valued {{tmath| x }}, the transform integral becomes a summation of sinusoids, which is still a continuous function of frequency ({{tmath| \xi }} or {{tmath| \omega }}).  When the sinusoids are harmonically related (i.e. when the <math>x</math>-values are spaced at integer multiples of an interval), the transform is called [[discrete-time Fourier transform]] (DTFT).

=== Discrete Fourier transforms and fast Fourier transforms ===
Sampling the DTFT at equally-spaced values of frequency is the most common modern method of computation.  Efficient procedures, depending on the frequency resolution needed, are described at {{section link|Discrete-time Fourier transform|Sampling the DTFT|nopage=n}}.  The [[discrete Fourier transform]] (DFT), used there, is usually computed by a [[fast Fourier transform]] (FFT) algorithm.

=== Symbolic integration of closed-form functions ===
Tables of [[closed-form expression|closed-form]] Fourier transforms, such as {{section link||Square-integrable functions, one-dimensional}} and {{section link|Discrete-time Fourier transform|Table of discrete-time Fourier transforms|nopage=y}}, are created by mathematically evaluating the Fourier analysis integral (or summation) into another closed-form function of frequency ({{tmath| \xi }} or {{tmath| \omega }}).<ref name="Zwillinger-2014">{{harvnb|Gradshteyn|Ryzhik|Geronimus|Tseytlin|2015}}</ref>  When mathematically possible, this provides a transform for a continuum of frequency values.

Many computer algebra systems such as [[Matlab]] and [[Mathematica]] that are capable of [[symbolic integration]] are capable of computing Fourier transforms symbolically.{{refn|group=note|For example, to compute the Fourier transform of {{math|1=cos(6π''t'') ''e''<sup>−π''t''<sup>2</sup></sup>}} one might enter the command {{code|integrate cos(6*pi*t) exp(−pi*t^2) exp(-i*2*pi*f*t) from -inf to inf}} into [[Wolfram Alpha]].  The direct command {{code|fourier transform of cos(6*pi*t) exp(−pi*t^2)}} would also work for Wolfram Alpha, although the options for the convention (see ''{{section link|#Other_conventions}}'') must be changed away from the default option, which is actually equivalent to {{code|integrate cos(6*pi*t) exp(−pi*t^2) exp(i*omega*t) /sqrt(2*pi) from -inf to inf}}.}}
https://en.wikipedia.org/wiki/Help:Edit_summary

=== Numerical integration of closed-form continuous functions ===
Discrete sampling of the Fourier transform can also be done by [[numerical integration]] of the definition at each value of frequency for which transform is desired.<ref>{{harvnb|Press|Flannery|Teukolsky|Vetterling|1992}}</ref><ref>{{harvnb|Bailey|Swarztrauber|1994}}</ref><ref>{{harvnb|Lado|1971}}</ref>  The numerical integration approach works on a much broader class of functions than the analytic approach.

=== Numerical integration of a series of ordered pairs ===
If the input function is a series of ordered pairs, numerical integration reduces to just a summation over the set of data pairs.<ref>{{harvnb|Simonen|Olkkonen|1985}}</ref>  The DTFT is a common subcase of this more general situation.

== Tables of important Fourier transforms ==
The following tables record some closed-form Fourier transforms. For functions {{math|''f''(''x'')}} and {{math|''g''(''x'')}} denote their Fourier transforms by {{math|''f̂''}} and {{math|''ĝ''}}. Only the three most common conventions are included. It may be useful to notice that entry 105 gives a relationship between the Fourier transform of a function and the original function, which can be seen as relating the Fourier transform and its inverse.

=== Functional relationships, one-dimensional ===
The Fourier transforms in this table may be found in {{harvtxt|Erdélyi|1954}} or {{harvtxt|Kammler|2000|loc=appendix}}.
{| class="wikitable"
! !! Function !! Fourier transform {{br}} unitary, ordinary frequency !! Fourier transform {{br}} unitary, angular frequency !! Fourier transform {{br}} non-unitary, angular frequency !!Remarks
|-
|
|<math> f(x)</math>
|<math>\begin{align} &\widehat f(\xi) \triangleq \widehat f_1(\xi) \\&= \int_{-\infty}^\infty f(x) e^{-i 2\pi \xi x}\, dx \end{align}</math>
|<math>\begin{align} &\widehat f(\omega) \triangleq \widehat f_2(\omega) \\&= \frac{1}{\sqrt{2 \pi}} \int_{-\infty}^\infty f(x) e^{-i \omega x}\, dx \end{align}</math>
|<math>\begin{align} &\widehat f(\omega) \triangleq \widehat f_3(\omega) \\&= \int_{-\infty}^\infty f(x) e^{-i \omega x}\, dx \end{align}</math>
|Definitions
|-
| 101
|<math> a\, f(x) + b\, g(x)</math>
|<math> a\, \widehat{f}(\xi) + b\, \widehat{g}(\xi)</math>
|<math> a\, \widehat{f}(\omega) + b\, \widehat{g}(\omega)</math>
|<math> a\, \widehat{f}(\omega) + b\, \widehat{g}(\omega)</math>
|Linearity
|-
| 102
|<math> f(x - a)</math>
|<math> e^{-i 2\pi \xi a} \widehat{f}(\xi)</math>
|<math> e^{- i a \omega} \widehat{f}(\omega)</math>
|<math> e^{- i a \omega} \widehat{f}(\omega)</math>
|Shift in time domain
|-
| 103
|<math> f(x)e^{iax}</math>
|<math> \widehat{f} \left(\xi - \frac{a}{2\pi}\right)</math>
|<math> \widehat{f}(\omega - a)</math>
|<math> \widehat{f}(\omega - a)</math>
|Shift in frequency domain, dual of 102
|-
| 104
|<math> f(a x)</math>
|<math> \frac{1}{|a|} \widehat{f}\left( \frac{\xi}{a} \right)</math>
|<math> \frac{1}{|a|} \widehat{f}\left( \frac{\omega}{a} \right)</math>
|<math> \frac{1}{|a|} \widehat{f}\left( \frac{\omega}{a} \right)</math>
|Scaling in the time domain. If {{math|{{abs|''a''}}}} is large, then {{math|''f''(''ax'')}} is concentrated around {{math|0}} and <math display="inline"> \frac{1}{|a|}\widehat{f} \left( \frac{\omega}{a} \right)</math> spreads out and flattens.
|-
| 105
|<math> \widehat f_n(x)</math>
|<math> \widehat f_1(x) \ \stackrel{\mathcal{F}_1}{\longleftrightarrow}\  f(-\xi)</math>
|<math> \widehat f_2(x) \ \stackrel{\mathcal{F}_2}{\longleftrightarrow}\  f(-\omega)</math>
|<math> \widehat f_3(x) \ \stackrel{\mathcal{F}_3}{\longleftrightarrow}\ 2\pi f(-\omega)</math>
|The same transform is applied twice, but {{math|''x''}} replaces the frequency variable ({{math|''ξ''}} or {{math|''ω''}}) after the first transform.
|-
| 106
|<math> \frac{d^n f(x)}{dx^n}</math>
|<math> (i 2\pi \xi)^n \widehat{f}(\xi)</math>
|<math> (i\omega)^n \widehat{f}(\omega)</math>
|<math> (i\omega)^n \widehat{f}(\omega)</math>
|{{math|''n''}}th-order derivative.
As {{math|''f''}} is a [[Schwartz space|Schwartz function]]
|-
|106.5
|<math>\int_{-\infty}^{x} f(\tau) d \tau</math>
|<math>\frac{\widehat{f}(\xi)}{i 2 \pi \xi} + C \, \delta(\xi)</math>
|<math>\frac{\widehat{f} (\omega)}{i\omega} + \sqrt{2 \pi} C \delta(\omega)</math>
|<math>\frac{\widehat{f} (\omega)}{i\omega} + 2 \pi C \delta(\omega)</math>
|Integration.<ref>{{Cite web |date=2015 |orig-date=2010 |title=The Integration Property of the Fourier Transform |url=https://www.thefouriertransform.com/transform/integration.php |url-status=live |archive-url=https://web.archive.org/web/20220126171340/https://www.thefouriertransform.com/transform/integration.php |archive-date=2022-01-26 |access-date=2023-08-20 |website=The Fourier Transform .com}}</ref> Note: <math>\delta</math> is the [[Dirac delta function]] and <math>C</math> is the average ([[DC component|DC]]) value of <math>f(x)</math> such that <math display="inline">\int_{-\infty}^\infty (f(x) - C) \, dx = 0</math>
|-
| 107
|<math> x^n f(x)</math>
|<math> \left (\frac{i}{2\pi}\right)^n \frac{d^n \widehat{f}(\xi)}{d\xi^n}</math>
|<math> i^n \frac{d^n \widehat{f}(\omega)}{d\omega^n}</math>
|<math> i^n \frac{d^n \widehat{f}(\omega)}{d\omega^n}</math>
|This is the dual of 106
|-
| 108
|<math> (f * g)(x)</math>
|<math> \widehat{f}(\xi) \widehat{g}(\xi)</math>
|<math> \sqrt{2\pi}\ \widehat{f}(\omega) \widehat{g}(\omega)</math>
|<math> \widehat{f}(\omega) \widehat{g}(\omega)</math>
|The notation {{math|''f'' ∗ ''g''}} denotes the [[convolution]] of {{mvar|f}} and {{mvar|g}} – this rule is the [[convolution theorem]]
|-
| 109
|<math> f(x) g(x)</math>
|<math> \left(\widehat{f} * \widehat{g}\right)(\xi)</math>
|<math> \frac{1}\sqrt{2\pi}\left(\widehat{f} * \widehat{g}\right)(\omega)</math>
|<math> \frac{1}{2\pi}\left(\widehat{f} * \widehat{g}\right)(\omega)</math>
|This is the dual of 108
|-
| 110
|For {{math|''f''(''x'')}} purely real
|<math> \widehat{f}(-\xi) = \overline{\widehat{f}(\xi)}</math>
|<math> \widehat{f}(-\omega) = \overline{\widehat{f}(\omega)}</math>
|<math> \widehat{f}(-\omega) = \overline{\widehat{f}(\omega)}</math>
|Hermitian symmetry. {{math|{{overline|''z''}}}} indicates the [[complex conjugate]].
|-
<!-- A Symmetry section has been added instead of this.
| 111
|For {{math|''f''(''x'')}} purely real and [[even function|even]]
| colspan=3 align=center |<math>\widehat f </math> is a purely real and [[even function]].
|
|-
| 112
|For {{math|''f''(''x'')}} purely real and [[odd function|odd]]
| colspan=3 align=center |<math>\widehat f </math> is a purely [[imaginary number|imaginary]] and [[odd function]].
|
|-->
| 113
|For {{math|''f''(''x'')}} purely imaginary
|<math> \widehat{f}(-\xi) = -\overline{\widehat{f}(\xi)}</math>
|<math> \widehat{f}(-\omega) = -\overline{\widehat{f}(\omega)}</math>
|<math> \widehat{f}(-\omega) = -\overline{\widehat{f}(\omega)}</math>
|{{math|{{overline|''z''}}}} indicates the [[complex conjugate]].
|-
| 114
| <math> \overline{f(x)}</math>|| <math> \overline{\widehat{f}(-\xi)}</math> || <math> \overline{\widehat{f}(-\omega)}</math> || <math> \overline{\widehat{f}(-\omega)}</math> || [[Complex conjugate|Complex conjugation]], generalization of 110 and 113
|-
|115
|<math> f(x) \cos (a x)</math>
|<math> \frac{ \widehat{f}{\left(\xi - \frac{a}{2\pi}\right)} + \widehat{f}{\left(\xi+\frac{a}{2\pi}\right)}}{2}</math>
|<math> \frac{\widehat{f}(\omega-a)+\widehat{f}(\omega+a)}{2}</math>
|<math> \frac{\widehat{f}(\omega-a)+\widehat{f}(\omega+a)}{2}</math>
|This follows from rules 101 and 103 using [[Euler's formula]]: {{tmath|1= \cos(a x) = \tfrac{e^{i a x} + e^{-i a x} }{2} }}.
|-
|116
|<math> f(x)\sin( ax)</math>
|<math> \frac{\widehat{f}{\left(\xi-\frac{a}{2\pi}\right)} - \widehat{f}{\left(\xi+\frac{a}{2\pi}\right)}}{2i}</math>
|<math> \frac{\widehat{f}(\omega-a)-\widehat{f}(\omega+a)}{2i}</math>
|<math> \frac{\widehat{f}(\omega-a)-\widehat{f}(\omega+a)}{2i}</math>
|This follows from 101 and 103 using [[Euler's formula]]: {{tmath|1= \sin(a x) = \tfrac{e^{i a x} - e^{-i a x} }{2i} }}.
|}

=== Square-integrable functions, one-dimensional ===
The Fourier transforms in this table may be found in {{harvtxt|Campbell|Foster|1948}}, {{harvtxt|Erdélyi|1954}}, or {{harvtxt|Kammler|2000|loc=appendix}}.
{| class="wikitable"
! !! Function !! Fourier transform {{br}} unitary, ordinary frequency !! Fourier transform {{br}} unitary, angular frequency !! Fourier transform {{br}} non-unitary, angular frequency !! Remarks
|-
|
|<math> f(x)</math>
|<math>\begin{align} &\widehat{f}(\xi) \triangleq \widehat f_1(\xi) \\&= \int_{-\infty}^\infty f(x) e^{-i 2\pi \xi x}\, dx \end{align}</math>
|<math>\begin{align} &\widehat{f}(\omega) \triangleq \widehat f_2(\omega) \\&= \frac{1}{\sqrt{2 \pi}} \int_{-\infty}^\infty f(x) e^{-i \omega x}\, dx \end{align}</math>
|<math>\begin{align} &\widehat{f}(\omega) \triangleq \widehat f_3(\omega) \\&= \int_{-\infty}^\infty f(x) e^{-i \omega x}\, dx \end{align}</math>
|Definitions
|-
|{{anchor|rect}} 201
|<math> \operatorname{rect}(a x) </math>
|<math> \frac{1}{|a|}\, \operatorname{sinc}\left(\frac{\xi}{a}\right)</math>
|<math> \frac{1}{\sqrt{2 \pi a^2}}\, \operatorname{sinc}\left(\frac{\omega}{2\pi a}\right)</math>
|<math> \frac{1}{|a|}\, \operatorname{sinc}\left(\frac{\omega}{2\pi a}\right)</math>
|The [[rectangular function|rectangular pulse]] and the ''normalized'' [[sinc function]], here defined as {{math|1=sinc(''x'') = {{sfrac|sin(π''x'')|π''x''}}}}
|-
| 202
|<math> \operatorname{sinc}(a x)</math>
|<math> \frac{1}{|a|}\, \operatorname{rect}\left(\frac{\xi}{a} \right)</math>
|<math> \frac{1}{\sqrt{2\pi a^2}}\, \operatorname{rect}\left(\frac{\omega}{2 \pi a}\right)</math>
|<math> \frac{1}{|a|}\, \operatorname{rect}\left(\frac{\omega}{2 \pi a}\right)</math>
|Dual of rule 201. The [[rectangular function]] is an ideal [[low-pass filter]], and the [[sinc function]] is the [[Anticausal system|non-causal]] impulse response of such a filter. The [[sinc function]] is defined here as {{math|1=sinc(''x'') = {{sfrac|sin(π''x'')|π''x''}}}}.
|-
| 203
|<math> \operatorname{sinc}^2 (a x)</math>
|<math> \frac{1}{|a|}\, \operatorname{tri} \left( \frac{\xi}{a} \right) </math>
|<math> \frac{1}{\sqrt{2\pi a^2}}\, \operatorname{tri} \left( \frac{\omega}{2\pi a} \right) </math>
|<math> \frac{1}{|a|}\, \operatorname{tri} \left( \frac{\omega}{2\pi a} \right) </math>
| The function {{math|tri(''x'')}} is the [[triangular function]]
|-
| 204
|<math> \operatorname{tri} (a x)</math>
|<math> \frac{1}{|a|}\, \operatorname{sinc}^2 \left( \frac{\xi}{a} \right) </math>
|<math> \frac{1}{\sqrt{2\pi a^2}} \, \operatorname{sinc}^2 \left( \frac{\omega}{2\pi a} \right) </math>
|<math> \frac{1}{|a|} \, \operatorname{sinc}^2 \left( \frac{\omega}{2\pi a} \right) </math>
| Dual of rule 203.
|-
| 205
|<math> e^{- a x} u(x) </math>
|<math> \frac{1}{a + i 2\pi \xi}</math>
|<math> \frac{1}{\sqrt{2 \pi} (a + i \omega)}</math>
|<math> \frac{1}{a + i \omega}</math>
|The function {{math|''u''(''x'')}} is the [[Heaviside step function|Heaviside unit step function]] and {{math|''a'' > 0}}.
|-
| 206
|<math> e^{-\alpha x^2}</math>
|<math> \sqrt{\frac{\pi}{\alpha}}\, e^{-\frac{(\pi \xi)^2}{\alpha}}</math>
|<math> \frac{1}{\sqrt{2 \alpha}}\, e^{-\frac{\omega^2}{4 \alpha}}</math>
|<math> \sqrt{\frac{\pi}{\alpha}}\, e^{-\frac{\omega^2}{4 \alpha}}</math>
|This shows that, for the unitary Fourier transforms, the [[Gaussian function]] {{math|''e''<sup>−''αx''<sup>2</sup></sup>}} is its own Fourier transform for some choice of {{mvar|α}}. For this to be integrable we must have {{math|Re(''α'') > 0}}.
|-
| 208
|<math> e^{-a|x|} </math>
|<math> \frac{2 a}{a^2 + 4 \pi^2 \xi^2} </math>
|<math> \sqrt{\frac{2}{\pi}} \, \frac{a}{a^2 + \omega^2} </math>
|<math> \frac{2a}{a^2 + \omega^{2}} </math>
|For {{math|Re(''a'') > 0}}. That is, the Fourier transform of a [[Laplace distribution|two-sided decaying exponential function]] is a [[Lorentzian function]].
|-
| 209
|<math> \operatorname{sech}(a x) </math>
|<math> \frac{\pi}{a} \operatorname{sech} \left( \frac{\pi^2}{ a} \xi \right)</math>
|<math> \frac{1}{a}\sqrt{\frac{\pi}{2}} \operatorname{sech}\left( \frac{\pi}{2 a} \omega \right)</math>
|<math> \frac{\pi}{a}\operatorname{sech}\left( \frac{\pi}{2 a} \omega \right)</math>
|[[Hyperbolic function|Hyperbolic secant]] is its own Fourier transform
|-
| 210
|<math> e^{-\frac{a^2 x^2}2} H_n(a x)</math>
|<math> \frac{\sqrt{2\pi}(-i)^n}{a} e^{-\frac{2\pi^2\xi^2}{a^2}} H_n{\left(\frac{2\pi\xi}a\right)}</math>
|<math> \frac{(-i)^n}{a} e^{-\frac{\omega^2}{2 a^2}} H_n{\left(\frac \omega a\right)}</math>
|<math> \frac{(-i)^n \sqrt{2\pi}}{a} e^{-\frac{\omega^2}{2 a^2}} H_n{\left(\frac \omega a \right)}</math>
|{{math|''H<sub>n</sub>''}} is the {{mvar|n}}th-order [[Hermite polynomial]]. If {{math|''a'' {{=}} 1}} then the Gauss–Hermite functions are [[eigenfunction]]s of the Fourier transform operator. For a derivation, see ''{{section link|Hermite polynomials#Hermite functions as eigenfunctions of the Fourier transform}}''. The formula reduces to 206 for {{math|''n'' {{=}} 0}}.
|}

=== Distributions, one-dimensional ===
The Fourier transforms in this table may be found in {{harvtxt|Erdélyi|1954}} or {{harvtxt|Kammler|2000|loc=appendix}}.
{| class="wikitable"
! !! Function !! Fourier transform {{br}} unitary, ordinary frequency !! Fourier transform {{br}} unitary, angular frequency !! Fourier transform {{br}} non-unitary, angular frequency !! Remarks
|-
|
|<math> f(x)</math>
|<math>\begin{align} &\widehat{f}(\xi) \triangleq \widehat f_1(\xi) \\&= \int_{-\infty}^\infty f(x) e^{-i 2\pi \xi x}\, dx \end{align}</math>
|<math>\begin{align} &\widehat{f}(\omega) \triangleq \widehat f_2(\omega) \\&= \frac{1}{\sqrt{2 \pi}} \int_{-\infty}^\infty f(x) e^{-i \omega x}\, dx \end{align}</math>
|<math>\begin{align} &\widehat{f}(\omega) \triangleq \widehat f_3(\omega) \\&= \int_{-\infty}^\infty f(x) e^{-i \omega x}\, dx \end{align}</math>
|Definitions
|-
| 301
|<math> 1</math>
|<math> \delta(\xi)</math>
|<math> \sqrt{2\pi}\, \delta(\omega)</math>
|<math> 2\pi\delta(\omega)</math>
|The distribution {{math|''δ''(''ξ'')}} denotes the [[Dirac delta function]].
|-
| 302
|<math> \delta(x)</math>
|<math> 1</math>
|<math> \frac{1}{\sqrt{2\pi}}</math>
|<math> 1</math>
|Dual of rule 301.
|-
| 303
|<math> e^{i a x}</math>
|<math> \delta\left(\xi - \frac{a}{2\pi}\right)</math>
|<math> \sqrt{2 \pi}\, \delta(\omega - a)</math>
|<math> 2 \pi\delta(\omega - a)</math>
|This follows from 103 and 301.
|-
| 304
|<math> \cos (a x)</math>
|<math> \frac{ \delta{\left(\xi - \frac{a}{2\pi}\right)} + \delta{\left(\xi+\frac{a}{2\pi}\right)}}{2}</math>
|<math> \sqrt{2 \pi}\,\frac{\delta(\omega-a)+\delta(\omega+a)}{2}</math>
|<math> \pi\left(\delta(\omega-a)+\delta(\omega+a)\right)</math>
|This follows from rules 101 and 303 using [[Euler's formula]]: {{tmath|1= \cos(a x) = \tfrac{e^{i a x} + e^{-i a x} }{2} }}.
|-
| 305
|<math> \sin( ax)</math>
|<math> \frac{\delta{\left(\xi-\frac{a}{2\pi}\right)} - \delta{\left(\xi+\frac{a}{2\pi}\right)}}{2i}</math>
|<math> \sqrt{2 \pi}\,\frac{\delta(\omega-a)-\delta(\omega+a)}{2i}</math>
|<math> i\pi\bigl(\delta(\omega+a)-\delta(\omega-a)\bigr)</math>
|This follows from 101 and 303 using {{tmath|1= \sin(a x) = \tfrac{e^{i a x} - e^{-i a x} }{2i} }}.
|-
| 306
|<math> \cos \left( a x^2 \right) </math>
|<math> \sqrt{\frac{\pi}{a}} \cos \left( \frac{\pi^2 \xi^2}{a} - \frac{\pi}{4} \right) </math>
|<math> \frac{1}{\sqrt{2 a}} \cos \left( \frac{\omega^2}{4 a} - \frac{\pi}{4} \right) </math>
|<math> \sqrt{\frac{\pi}{a}} \cos \left( \frac{\omega^2}{4a} - \frac{\pi}{4} \right) </math>
|This follows from 101 and 207 using {{tmath|1= \cos(a x^2) = \tfrac{e^{i a x^2} + e^{-i a x^2} }{2} }}.
|-
| 307
|<math> \sin \left( a x^2 \right) </math>
|<math> - \sqrt{\frac{\pi}{a}} \sin \left( \frac{\pi^2 \xi^2}{a} - \frac{\pi}{4} \right) </math>
|<math> \frac{-1}{\sqrt{2 a}} \sin \left( \frac{\omega^2}{4 a} - \frac{\pi}{4} \right) </math>
|<math> -\sqrt{\frac{\pi}{a}}\sin \left( \frac{\omega^2}{4a} - \frac{\pi}{4} \right)</math>
|This follows from 101 and 207 using {{tmath|1= \sin(a x^2) = \tfrac{e^{i a x^2} - e^{-i a x^2} }{2i} }}.
|-
|308
|<math> e^{-\pi i\alpha x^2}</math>
|<math> \frac{1}{\sqrt{\alpha}}\, e^{-i\frac{\pi}{4}} e^{i\frac{\pi \xi^2}{\alpha}}</math>
|<math> \frac{1}{\sqrt{2\pi \alpha}}\, e^{-i\frac{\pi}{4}} e^{i\frac{\omega^2}{4\pi \alpha}}</math>
|<math> \frac{1}{\sqrt{\alpha}}\, e^{-i\frac{\pi}{4}} e^{i\frac{\omega^2}{4\pi \alpha}}</math>
|Here it is assumed <math>\alpha</math> is real. For the case that alpha is complex see table entry 206 above.
|-
| 309
|<math> x^n</math>
|<math> \left(\frac{i}{2\pi}\right)^n \delta^{(n)} (\xi)</math>
|<math> i^n \sqrt{2\pi} \delta^{(n)} (\omega)</math>
|<math> 2\pi i^n\delta^{(n)} (\omega)</math>
|Here, {{mvar|n}} is a [[natural number]] and {{math|''δ''{{isup|(''n'')}}(''ξ'')}} is the {{mvar|n}}th distribution derivative of the Dirac delta function. This rule follows from rules 107 and 301. Combining this rule with 101, we can transform all [[polynomial]]s.
|-
| 310
|<math> \delta^{(n)}(x)</math>
|<math> (i 2\pi \xi)^n</math>
|<math> \frac{(i\omega)^n}{\sqrt{2\pi}} </math>
|<math> (i\omega)^n</math>
|Dual of rule 309. {{math|''δ''{{isup|(''n'')}}(''ξ'')}} is the {{mvar|n}}th distribution derivative of the Dirac delta function. This rule follows from 106 and 302.
|-
| 311
|<math> \frac{1}{x}</math>
|<math> -i\pi\sgn(\xi)</math>
|<math> -i\sqrt{\frac{\pi}{2}}\sgn(\omega)</math>
|<math> -i\pi\sgn(\omega)</math>
|Here {{math|sgn(''ξ'')}} is the [[sign function]]. Note that {{math|{{sfrac|1|''x''}}}} is not a distribution. It is necessary to use the [[Cauchy principal value]] when testing against [[Schwartz functions]]. This rule is useful in studying the [[Hilbert transform]].
|-
| 312
|<math>\begin{align}
&\frac{1}{x^n} \\
&:= \frac{(-1)^{n-1}}{(n-1)!}\frac{d^n}{dx^n}\log |x|
\end{align}</math>
|<math> -i\pi \frac{(-i 2\pi \xi)^{n-1}}{(n-1)!} \sgn(\xi)</math>
|<math> -i\sqrt{\frac{\pi}{2}}\, \frac{(-i\omega)^{n-1}}{(n-1)!}\sgn(\omega)</math>
|<math> -i\pi \frac{(-i\omega)^{n-1}}{(n-1)!}\sgn(\omega)</math>
|{{math|{{sfrac|1|''x''<sup>''n''</sup>}}}} is the [[homogeneous distribution]] defined by the distributional derivative{{br}}<math>\tfrac{(-1)^{n-1}}{(n-1)!}\tfrac{d^n}{dx^n}\log|x|</math>
|-
| 313
|<math> |x|^\alpha</math>
|<math> -\frac{2\sin\left(\frac{\pi\alpha}{2}\right)\Gamma(\alpha+1)}{|2\pi\xi|^{\alpha+1}}</math>
|<math> \frac{-2}{\sqrt{2\pi}}\, \frac{\sin\left(\frac{\pi\alpha}{2}\right)\Gamma(\alpha+1)}{|\omega|^{\alpha+1}} </math>
|<math> -\frac{2\sin\left(\frac{\pi\alpha}{2}\right)\Gamma(\alpha+1)}{|\omega|^{\alpha+1}} </math>
|This formula is valid for {{math|−1 < ''α'' < 0}}. For {{math|''α'' > 0}} some singular terms arise at the origin that can be found by differentiating 320. If {{math|Re ''α'' > −1}}, then {{math|{{abs|''x''}}<sup>''α''</sup>}} is a locally integrable function, and so a tempered distribution. The function {{math|''α'' ↦ {{abs|''x''}}<sup>''α''</sup>}} is a holomorphic function from the right half-plane to the space of tempered distributions. It admits a unique meromorphic extension to a tempered distribution, also denoted {{math|{{abs|''x''}}<sup>''α''</sup>}} for {{math|''α'' ≠ −1, −3, ...}} (see ''[[Homogeneous distribution]]'').
|-
| <!-- Should we call it 313a ? Doesn't necessarily need a number, because it is a special case. -->
|<math> \frac{1}{\sqrt{|x|}} </math>
|<math> \frac{1}{\sqrt{|\xi|}} </math>
|<math> \frac{1}{\sqrt{|\omega|}}</math>
|<math> \frac{\sqrt{2\pi}}{\sqrt{|\omega|}} </math>
| Special case of 313
|-
| 314
|<math> \sgn(x)</math>
|<math> \frac{1}{i\pi \xi}</math>
|<math> \sqrt{\frac{2}{\pi}} \frac{1}{i\omega } </math>
|<math> \frac{2}{i\omega }</math>
|The dual of rule 311. This time the Fourier transforms need to be considered as a [[Cauchy principal value]].
|-
| 315
|<math> u(x)</math>
|<math> \frac{1}{2}\left(\frac{1}{i \pi \xi} + \delta(\xi)\right)</math>
|<math> \sqrt{\frac{\pi}{2}} \left( \frac{1}{i \pi \omega} + \delta(\omega)\right)</math>
|<math> \pi\left( \frac{1}{i \pi \omega} + \delta(\omega)\right)</math>
|The function {{math|''u''(''x'')}} is the Heaviside [[Heaviside step function|unit step function]]; this follows from rules 101, 301, and 314.
|-
| 316
|<math> \sum_{n=-\infty}^{\infty} \delta (x - n T)</math>
|<math> \frac{1}{T} \sum_{k=-\infty}^{\infty} \delta{\left( \xi -\frac{k }{T}\right)}</math>
|<math> \frac{\sqrt{2\pi }}{T}\sum_{k=-\infty}^{\infty} \delta{\left( \omega -\frac{2\pi k}{T}\right)}</math>
|<math> \frac{2\pi}{T}\sum_{k=-\infty}^{\infty} \delta{\left( \omega -\frac{2\pi k}{T}\right)}</math>
|This function is known as the [[Dirac comb]] function. This result can be derived from 302 and 102, together with the fact that <math display="inline">\sum_{n=-\infty}^{\infty} e^{inx}</math> <math display="inline">= 2\pi\sum_{k=-\infty}^{\infty} \delta(x+2\pi k) </math> as distributions.
|-
| 317
|<math> J_0 (x)</math>
|<math> \frac{2\, \operatorname{rect}(\pi\xi)}{\sqrt{1 - 4 \pi^2 \xi^2}} </math>
|<math> \sqrt{\frac{2}{\pi}} \, \frac{\operatorname{rect}\left(  \frac{\omega}{2} \right)}{\sqrt{1 - \omega^2}} </math>
|<math> \frac{2\,\operatorname{rect}\left(\frac{\omega}{2} \right)}{\sqrt{1 - \omega^2}}</math>
| The function {{math|''J''<sub>0</sub>(''x'')}} is the zeroth order [[Bessel function]] of first kind.
|-
| 318
|<math> J_n (x)</math>
|<math> \frac{2 (-i)^n T_n (2 \pi \xi) \operatorname{rect}(\pi \xi)}{\sqrt{1 - 4 \pi^2 \xi^2}} </math>
|<math> \sqrt{\frac{2}{\pi}} \frac{ (-i)^n T_n (\omega) \operatorname{rect} \left( \frac{\omega}{2} \right)}{\sqrt{1 - \omega^2}} </math>
|<math> \frac{2(-i)^n T_n (\omega) \operatorname{rect} \left( \frac{\omega}{2} \right)}{\sqrt{1 - \omega^2}} </math>
| This is a generalization of 317. The function {{math|''J<sub>n</sub>''(''x'')}} is the {{mvar|n}}th order [[Bessel function]] of first kind. The function {{math|''T<sub>n</sub>''(''x'')}} is the [[Chebyshev polynomials|Chebyshev polynomial of the first kind]].
|-
| 319
|<math> \log \left| x \right|</math>
|<math> -\frac{1}{2} \frac{1}{\left| \xi \right|} - \gamma \delta \left( \xi \right) </math>
|<math> -\frac{\sqrt\frac{\pi}{2}}{\left| \omega \right|} - \sqrt{2 \pi} \gamma \delta \left( \omega \right) </math>
|<math> -\frac{\pi}{\left| \omega \right|} - 2 \pi \gamma \delta \left( \omega \right) </math>
|{{mvar|γ}} is the [[Euler–Mascheroni constant]]. It is necessary to use a finite part integral when testing {{math|{{sfrac|1|{{abs|''ξ''}}}}}} or {{math|{{sfrac|1|{{abs|''ω''}}}}}}against [[Schwartz functions]]. The details of this might change the coefficient of the delta function.
|- 
| 320
|<math> \left( \mp ix \right)^{-\alpha}</math>
|<math> \frac{\left(2\pi\right)^\alpha}{\Gamma\left(\alpha\right)}u\left(\pm \xi \right)\left(\pm \xi \right)^{\alpha-1} </math>
|<math> \frac{\sqrt{2\pi}}{\Gamma\left(\alpha\right)}u\left(\pm\omega\right)\left(\pm\omega\right)^{\alpha-1} </math>
|<math> \frac{2\pi}{\Gamma\left(\alpha\right)}u\left(\pm\omega\right)\left(\pm\omega\right)^{\alpha-1} </math>
|This formula is valid for {{math|0 < ''α'' < 1}}. Use differentiation to derive formula for higher exponents. {{mvar|u}} is the Heaviside function.
|}

=== Two-dimensional functions ===
{| class="wikitable"
! !! Function !! Fourier transform {{br}} unitary, ordinary frequency !! Fourier transform {{br}} unitary, angular frequency !! Fourier transform {{br}} non-unitary, angular frequency !! Remarks
|-
|400
|<math> f(x,y)</math>
|<math>\begin{align}& \widehat{f}(\xi_x, \xi_y)\triangleq \\ & \iint f(x,y) e^{-i 2\pi(\xi_x x+\xi_y y)}\,dx\,dy \end{align}</math>
|<math>\begin{align}& \widehat{f}(\omega_x,\omega_y)\triangleq \\ & \frac{1}{2 \pi} \iint f(x,y) e^{-i (\omega_x x +\omega_y y)}\, dx\,dy  \end{align}</math>
|<math>\begin{align}& \widehat{f}(\omega_x,\omega_y)\triangleq \\ & \iint f(x,y) e^{-i(\omega_x x+\omega_y y)}\, dx\,dy  \end{align}</math>
|The variables {{mvar|ξ<sub>x</sub>}}, {{mvar|ξ<sub>y</sub>}}, {{mvar|ω<sub>x</sub>}}, {{mvar|ω<sub>y</sub>}} are real numbers. The integrals are taken over the entire plane.
|-
|401
|<math> e^{-\pi\left(a^2x^2+b^2y^2\right)}</math>
|<math> \frac{1}{|ab|} e^{-\pi\left(\frac{\xi_x^2}{a^2} + \frac{\xi_y^2}{b^2}\right)}</math>
|<math> \frac{1}{2\pi\,|ab|} e^{-\frac{1}{4\pi}\left(\frac{\omega_x^2}{a^2} + \frac{\omega_y^2}{b^2}\right)}</math>
|<math> \frac{1}{|ab|} e^{-\frac{1}{4\pi}\left(\frac{\omega_x^2}{a^2} + \frac{\omega_y^2}{b^2}\right)}</math>
|Both functions are Gaussians, which may not have unit volume.
|-
|402
|<math> \operatorname{circ}\left(\sqrt{x^2+y^2}\right)</math>
|<math> \frac{J_1\left(2 \pi \sqrt{\xi_x^2+\xi_y^2}\right)}{\sqrt{\xi_x^2+\xi_y^2}}</math>
|<math> \frac{J_1\left(\sqrt{\omega_x^2+\omega_y^2}\right)}{\sqrt{\omega_x^2+\omega_y^2}}</math>
|<math> \frac{2\pi J_1\left(\sqrt{\omega_x^2+\omega_y^2}\right)}{\sqrt{\omega_x^2+\omega_y^2}}</math>
|The function is defined by {{math|1=circ(''r'') = 1}} for {{math|0 ≤ ''r'' ≤ 1}}, and is 0 otherwise. The result is the amplitude distribution of the [[Airy disk]], and is expressed using {{math|''J''<sub>1</sub>}} (the order-1 [[Bessel function]] of the first kind).<ref>{{harvnb|Stein|Weiss|1971|loc=Thm. IV.3.3}}</ref>
|-
|403
|<math> \frac{1}{\sqrt{x^2+y^2}}</math>
|<math> \frac{1}{\sqrt{\xi_x^2+\xi_y^2}}</math>
|<math> \frac{1}{\sqrt{\omega_x^2+\omega_y^2}}</math>
|<math> \frac{2\pi}{\sqrt{\omega_x^2+\omega_y^2}}</math>
|This is the [[Hankel transform]] of {{math|1=''r''<sup>−1</sup>}}, a 2-D Fourier "self-transform".<ref>{{harvnb|Easton|2010}}</ref>
|-
|404
|<math> \frac{i}{x+i y}</math>
|<math> \frac{1}{\xi_x+i\xi_y}</math>
|<math> \frac{1}{\omega_x+i\omega_y}</math>
|<math> \frac{2\pi}{\omega_x+i\omega_y}</math>
|<!--This formula was used in constructing the ground state wavefunction of two-dimensional <math> p_x+ip_y</math> superconductors<ref>Phys. Rev. B 97 (10), 104501 (2018)</ref>-->
|}

=== Formulas for general <span class="texhtml">''n''</span>-dimensional functions ===
{| class="wikitable"
! !! Function !! Fourier transform {{br}} unitary, ordinary frequency !! Fourier transform {{br}} unitary, angular frequency !! Fourier transform {{br}} non-unitary, angular frequency !! Remarks
|-
|500
|<math> f(\mathbf x)</math>
|<math>\begin{align} &\widehat f_1 (\boldsymbol \xi) \triangleq \\ &\int_{\mathbb{R}^n}f(\mathbf x) e^{-i 2\pi \boldsymbol \xi \cdot \mathbf x }\, d \mathbf x \end{align}</math>
|<math>\begin{align} &\widehat f_2 (\boldsymbol \omega) \triangleq \\ &\frac{1}{{(2 \pi)}^\frac{n}{2}} \int_{\mathbb{R}^n} f(\mathbf x) e^{-i \boldsymbol \omega \cdot \mathbf x}\, d \mathbf x \end{align}</math>
|<math>\begin{align} &\widehat f_3 (\boldsymbol \omega) \triangleq \\ &\int_{\mathbb{R}^n}f(\mathbf x) e^{-i \boldsymbol \omega \cdot \mathbf x}\, d \mathbf x \end{align}</math>
|
|-
|501
|<math> \chi_{[0,1]}(|\mathbf x|)\left(1-|\mathbf x|^2\right)^\delta</math>
|<math> \frac{\Gamma(\delta+1)}{\pi^\delta\,|\boldsymbol \xi|^\gamma}  J_{\gamma}(2\pi|\boldsymbol \xi|)</math>
|<math> 2^\delta \, \frac{\Gamma(\delta+1)}{\left|\boldsymbol \omega\right|^\gamma}  J_{\gamma}(|\boldsymbol \omega|)</math>
|<math> \frac{\Gamma(\delta+1)}{\pi^\delta} \left|\frac{\boldsymbol \omega}{2\pi}\right|^{-\gamma} J_{\gamma}(\!|\boldsymbol \omega|\!)</math>
|Here, <math>\gamma = \tfrac{n}{2} + \delta</math>.
The function {{math|''χ''<sub>[0, 1]</sub>}} is the [[indicator function]] of the interval {{math|[0, 1]}}. The function {{math|Γ(''x'')}} is the gamma function. The function {{math|''J''<sub>{{sfrac|''n''|2}}+''δ''</sub>}} is a Bessel function of the first kind, with order {{math|{{sfrac|''n''|2}} + ''δ''}}. Taking {{math|1=''n'' = 2}} and {{math|1=''δ'' = 0}} produces 402.<ref>{{harvnb|Stein|Weiss|1971|loc=Thm. 4.15}}</ref>
|-
|502
|<math> |\mathbf x|^{-\alpha}, \quad 0 < \operatorname{Re} \alpha < n</math>
|<math> \frac{(2\pi)^{\alpha}}{c_{n, \alpha}} |\boldsymbol \xi|^{-(n - \alpha)}</math>
|<math> \frac{(2\pi)^{\frac{n}{2}}}{c_{n, \alpha}} |\boldsymbol \omega|^{-(n - \alpha)}</math>
|<math> \frac{(2\pi)^{n}}{c_{n, \alpha}} |\boldsymbol \omega|^{-(n - \alpha)}</math>
|See ''[[Riesz potential]]'', where the constant is given by {{tmath|1= \textstyle c_{n, \alpha} = \pi^\tfrac{n}{2} 2^\alpha {\Gamma\left(\frac{\alpha}{2}\right)}/{\Gamma\left(\frac{n - \alpha}{2}\right)} }}. The formula also holds for all {{math|''α'' ≠ ''n'', ''n'' + 2, ...}} by analytic continuation, but then the function and its Fourier transforms need to be understood as suitably regularized tempered distributions (see ''[[Homogeneous distribution]]'').{{refn|group=note|In {{harvnb|Gelfand|Shilov|1964|p=363}}, with the non-unitary conventions of this table, the transform of <math>|\mathbf x|^\lambda</math> is given to be {{tmath| \textstyle 2^{\lambda+n}\pi^{\tfrac12 n}{\Gamma(\frac{\lambda+n}{2})}/{\Gamma(-\frac{\lambda}{2})}\vert\boldsymbol\omega\vert^{-\lambda-n} }} from which this follows, with {{tmath|1= \lambda=-\alpha }}.}}
|-
|503
|<math> \frac{1}{\left|\boldsymbol \sigma\right|\left(2\pi\right)^\frac{n}{2}} e^{-\frac{1}{2} \mathbf x^{\mathrm T} \boldsymbol \sigma^{-\mathrm T} \boldsymbol \sigma^{-1} \mathbf x}</math>
|<math> e^{-2\pi^2 \boldsymbol \xi^{\mathrm T} \boldsymbol \sigma \boldsymbol \sigma^{\mathrm T} \boldsymbol \xi} </math>
|<math> (2\pi)^{-\frac{n}{2}} e^{-\frac{1}{2} \boldsymbol \omega^{\mathrm T} \boldsymbol \sigma \boldsymbol \sigma^{\mathrm T} \boldsymbol \omega} </math>
|<math> e^{-\frac{1}{2} \boldsymbol \omega^{\mathrm T} \boldsymbol \sigma \boldsymbol \sigma^{\mathrm T} \boldsymbol \omega} </math>
|This is the formula for a [[multivariate normal distribution]] normalized to 1 with a mean of 0. Bold variables are vectors or matrices. Following the notation of the aforementioned page, {{math|'''Σ''' {{=}} '''σ''' '''σ'''<sup>T</sup>}} and {{math|'''Σ'''<sup>−1</sup> {{=}} '''σ'''<sup>−T</sup> '''σ'''<sup>−1</sup>}}
|-
|504
|<math> e^{-2\pi\alpha|\mathbf x|}</math>
|<math>\frac{c_n\alpha}{\left(\alpha^2+|\boldsymbol{\xi}|^2\right)^\frac{n+1}{2}}</math>
|<math>\frac{c_n (2\pi)^{\frac{n+2}{2}} \alpha}{\left(4\pi^2\alpha^2+|\boldsymbol{\omega}|^2\right)^\frac{n+1}{2}}</math>
|<math>\frac{c_n (2\pi)^{n+1} \alpha}{\left(4\pi^2\alpha^2+|\boldsymbol{\omega}|^2\right)^\frac{n+1}{2}}</math>
|Here<ref>{{harvnb|Stein|Weiss|1971|p=6}}</ref> {{tmath|1= \textstyle c_n={\Gamma\left(\frac{n+1}{2}\right)}/{\pi^\frac{n+1}{2} } }}, {{math|Re(''α'') > 0}}
|}

== See also ==
{{div col|colwidth=22em}}
* {{annotated link|Analog signal processing}}
* {{annotated link|Beevers–Lipson strip}}
* {{annotated link|Constant-Q transform}}
* {{annotated link|DFT matrix}}
* {{annotated link|Discrete Fourier transform}}
* {{annotated link|Fast Fourier transform}}
* {{annotated link|Fourier integral operator}}
* {{annotated link|Fourier inversion theorem}}
* {{annotated link|Fourier multiplier}}
* {{annotated link|Fourier series}}
* {{annotated link|Fourier sine transform}}
* [[Fourier–Deligne transform]]
* [[Fourier–Mukai transform]]
* {{annotated link|Fractional Fourier transform}}
* [[Indirect Fourier transform]] 
* {{annotated link|Integral transform}}
** {{annotated link|Hankel transform}}
** {{annotated link|Hartley transform}}
* {{annotated link|Laplace transform}}
* {{annotated link|Least-squares spectral analysis}}
* [[Linear canonical transform]]
* [[List of Fourier-related transforms]]
* {{annotated link|Mellin transform}}
* {{annotated link|Multidimensional transform}}
* [[NGC 4622]] – Especially the image NGC 4622 Fourier transform {{math|1=''m'' = 2}}.
* {{annotated link|Nonlocal operator}}
* [[Quadratic Fourier transform]]
* {{annotated link|Quantum Fourier transform}}
* {{annotated link|Short-time Fourier transform}}
* {{annotated link|Spectral density}}
** {{annotated link|Spectral density estimation}}
* {{annotated link|Symbolic integration}}
* [[Time stretch dispersive Fourier transform]]
* {{annotated link|Transform (mathematics)}}
{{div col end}}

== Notes ==
{{reflist|group=note}}

== Citations ==
{{reflist|22em}}

== References ==
{{refbegin|2|indent=yes}}
<!-- DO NOT leave blank lines between list items, they create entirely new lists -->
* {{cite journal | last1=Ablowitz | first1=Mark J. | last2=Kaup | first2=David J. | last3=Newell | first3=Alan C. | last4=Segur | first4=Harvey | title=The Inverse Scattering Transform‐Fourier Analysis for Nonlinear Problems | journal=Studies in Applied Mathematics | volume=53 | issue=4 | date=1974 | issn=0022-2526 | doi=10.1002/sapm1974534249 | pages=249–315 | url=https://onlinelibrary.wiley.com/doi/10.1002/sapm1974534249 | access-date=2025-09-21| url-access=subscription }}
* {{citation
 | last1 = Arfken | first1 = George
 | title = Mathematical Methods for Physicists
 | date = 1985
 | publisher = Academic Press
 | isbn = 978-0-12-059820-5
 | edition = 3rd
 }}
* {{citation
 | last1 = Bailey
 | first1 = David H.
 | last2 = Swarztrauber
 | first2 = Paul N.
 | title = A fast method for the numerical evaluation of continuous Fourier and Laplace transforms
 | journal = [[SIAM Journal on Scientific Computing]]
 | volume = 15
 | issue = 5
 | year = 1994
 | pages = 1105–1110
 | doi = 10.1137/0915067
 | bibcode = 1994SJSC...15.1105B
 | url = http://crd.lbl.gov/~dhbailey/dhbpapers/fourint.pdf
 | citeseerx = 10.1.1.127.1534
 | access-date = 2017-11-01
 | archive-date = 2008-07-20
 | archive-url = https://web.archive.org/web/20080720002714/http://crd.lbl.gov/~dhbailey/dhbpapers/fourint.pdf
 }}
* {{citation | last=Billingsley | first=Patrick | title=Probability and measure | publisher=Wiley | publication-place=New York, NY | date=1995 | isbn=978-0-471-00710-4}}
* {{citation
 | editor-last = Boashash | editor-first = B.
 | title = Time–Frequency Signal Analysis and Processing: A Comprehensive Reference
 | publisher = Elsevier Science
 | location = Oxford
 | year = 2003
 | isbn = 978-0-08-044335-5
}}
* {{citation
 | last1 = Bochner | first1 = S. | author1-link = Salomon Bochner
 | last2 = Chandrasekharan | first2 = K. | author2-link = K. S. Chandrasekharan
 | title = Fourier Transforms
 | publisher = [[Princeton University Press]]
 | year = 1949
}}
* {{citation
 | last = Bracewell | first = R. N.
 | title = The Fourier Transform and Its Applications
 | edition = 3rd
 | location = Boston
 | publisher = McGraw-Hill
 | year = 2000
 | isbn = 978-0-07-116043-8
}}
* {{citation
 | last1 = Campbell | first1 = George
 | last2 = Foster | first2 = Ronald
 | title = Fourier Integrals for Practical Applications
 | publisher = D. Van Nostrand Company, Inc.
 | location = New York
 | year = 1948
}}
* {{citation
 | last1 = Celeghini | first1 = Enrico
 | last2 = Gadella | first2 = Manuel
 | last3 = del Olmo | first3 = Mariano A.
 | journal = Symmetry
 | date = 2021
 | volume = 13
 | issue = 5
 | title = Hermite Functions and Fourier Series
 | page = 853
 | doi = 10.3390/sym13050853
 | arxiv = 2007.10406
 | bibcode = 2021Symm...13..853C
 | doi-access = free
}}
* {{citation
 | last = Champeney | first = D.C.
 | title = A Handbook of Fourier Theorems
 | year = 1987
 | publisher = [[Cambridge University Press]]
 | bibcode = 1987hft..book.....C
}}
* {{citation | last=Chandrasekharan | first=Komaravolu | title=Classical Fourier Transforms | publisher=Springer Berlin Heidelberg | publication-place=Berlin, Heidelberg | date=1989 | isbn=978-3-540-50248-7 | doi=10.1007/978-3-642-74029-9 | url=http://link.springer.com/10.1007/978-3-642-74029-9| url-access=subscription }}
* {{citation
 | last = Chatfield
 | first = Chris
 | title = The Analysis of Time Series: An Introduction
 | year = 2004
 | edition = 6th
 | publisher = Chapman & Hall/CRC
 | series = Texts in Statistical Science
 | location = London
 | isbn = 978-0-203-49168-3
 | url = https://books.google.com/books?id=qKzyAbdaDFAC&q=%22Fourier+transform%22
}}
* {{citation
 | last1 = Clozel | first1 = Laurent
 | last2 = Delorme | first2 = Patrice
 | title = Sur le théorème de Paley-Wiener invariant pour les groupes de Lie réductifs réels 
 | date = 1985
 | journal = Comptes Rendus de l'Académie des Sciences, Série I
 | volume = 300
 | pages = 331–333
}}
* {{citation
 | last = Condon | first = E. U. | author-link = Edward Condon
 | title = Immersion of the Fourier transform in a continuous group of functional transformations
 | journal = [[PNAS|Proc. Natl. Acad. Sci.]]
 | volume = 23
 | issue = 3
 | pages = 158–164
 | year = 1937
 | doi=10.1073/pnas.23.3.158
 | pmid = 16588141
 | pmc = 1076889
 | bibcode = 1937PNAS...23..158C
 | doi-access = free
}}
* {{cite journal
 |last1=Correia |first1=L. B.
 |last2=Justo |first2=J. F.
 |last3=Angélico |first3=B. A.
 |title=Polynomial Adaptive Synchrosqueezing Fourier Transform: A method to optimize multiresolution
 |journal=Digital Signal Processing
 |date=2024
 |volume=150 |article-number=104526
 |doi=10.1016/j.dsp.2024.104526 |bibcode=2024DSPRJ.15004526C
}}
* {{citation
 | last1 = de Groot | first1 = Sybren R.
 | last2 = Mazur | first2 = Peter
 | title = Non-Equilibrium Thermodynamics
 | edition = 2nd
 | year = 1984
 | publisher = [[Dover Publications|Dover]]
 | location = New York
}}
* {{citation
 | last = Duoandikoetxea | first = Javier
 | title = Fourier Analysis
 | publisher = [[American Mathematical Society]]
 | year = 2001
 | isbn = 978-0-8218-2172-5
}}
* {{citation
 | last1 = Dym | first1 = H. | author1-link = Harry Dym
 | last2 = McKean | first2 = H.
 | title = Fourier Series and Integrals
 | publisher = [[Academic Press]]
 | year = 1985
 | isbn = 978-0-12-226451-1
}}
* {{citation
 | last = Easton
 | first = Roger L. Jr.
 | title = Fourier Methods in Imaging
 | date = 2010
 | publisher = John Wiley & Sons
 | isbn = 978-0-470-68983-7
 | url = https://books.google.com/books?id=wCoDDQAAQBAJ
 | access-date = 26 May 2020
 | language = en
}}
* {{cite book | last=Edwards | first=R. E. | title=Fourier Series | series=Graduate Texts in Mathematics | publisher=Springer New York | publication-place=New York, NY | volume=64 | date=1979 | isbn=978-1-4612-6210-7 | doi=10.1007/978-1-4612-6208-4}}
* {{cite book | last=Edwards | first=R. E. | title=Fourier Series | series=Graduate Texts in Mathematics | publisher=Springer New York | publication-place=New York, NY | volume=85 | date=1982 | isbn=978-1-4613-8158-7 | doi=10.1007/978-1-4613-8156-3}}
* {{citation
 | editor-last = Erdélyi | editor-first = Arthur
 | title = Tables of Integral Transforms
 | volume = 1
 | publisher = McGraw-Hill
 | year = 1954
}}
* {{citation
 | last = Feller | first = William | author-link = William Feller
 | title = An Introduction to Probability Theory and Its Applications
 | volume = II
 | publisher = [[John Wiley & Sons|Wiley]]
 | location = New York
 | edition = 2nd
 | mr = 0270403
 | year = 1971
}}
* {{citation
 | last = Folland | first = Gerald
 | title = Harmonic analysis in phase space
 | publisher = [[Princeton University Press]]
 | year = 1989
}}
* {{citation
 | last = Folland | first = Gerald
 | title = Fourier analysis and its applications
 | publisher = [[Wadsworth & Brooks/Cole]]
 | year = 1992
}}
* {{citation
 | last = Fourier | first = J.B. Joseph | author-link = Joseph Fourier
 | title = Théorie analytique de la chaleur
 | location = Paris
 | url = https://books.google.com/books?id=TDQJAAAAIAAJ&q=%22c%27est-%C3%A0-dire+qu%27on+a+l%27%C3%A9quation%22&pg=PA525
 | publisher = Firmin Didot, père et fils
 | year = 1822
 | language = fr
 | oclc = 2688081
}}
* {{citation
 | last = Fourier | first = J.B. Joseph | author-link = Joseph Fourier
 | title = The Analytical Theory of Heat
 | journal = Nature
 | url = https://books.google.com/books?id=-N8EAAAAYAAJ&q=%22that+is+to+say%2C+that+we+have+the+equation%22&pg=PA408
 | year = 1878
 | volume = 18
 | issue = 451
 | page = 192
 | orig-date = 1822
 | publisher = The University Press
 | doi = 10.1038/018192a0
 | bibcode = 1878Natur..18Q.192.
 | translator = Alexander Freeman
 | url-access = subscription
 }} (translated from French)
* {{citation
 | last1 = Gradshteyn | first1 = Izrail Solomonovich | author1-link = Izrail Solomonovich Gradshteyn
 | last2 = Ryzhik | first2 = Iosif Moiseevich | author2-link = Iosif Moiseevich Ryzhik
 | last3 = Geronimus | first3 = Yuri Veniaminovich | author3-link = Yuri Veniaminovich Geronimus
 | last4 = Tseytlin | first4 = Michail Yulyevich | author4-link = Michail Yulyevich Tseytlin
 | last5 = Jeffrey | first5 = Alan
 | editor1-last = Zwillinger | editor1-first = Daniel
 | editor2-last = Moll | editor2-first = Victor Hugo | editor-link2=Victor Hugo Moll 
 | translator = Scripta Technica, Inc.
 | title = Table of Integrals, Series, and Products
 | title-link = Gradshteyn and Ryzhik
 | publisher = [[Academic Press]]
 | year = 2015
 | edition = 8th
 | language = en
 | isbn = 978-0-12-384933-5
}}
* {{citation
 | last = Grafakos | first = Loukas
 | title = Classical and Modern Fourier Analysis
 | publisher = Prentice-Hall
 | year = 2004
 | isbn = 978-0-13-035399-3
}}
* {{citation
 | last1 = Grafakos | first1 = Loukas
 | last2 = Teschl | first2 = Gerald | author2-link = Gerald Teschl
 | title = On Fourier transforms of radial functions and distributions
 | journal = J. Fourier Anal. Appl.
 | volume = 19
 | pages = 167–179
 | year = 2013
 | issue = 1
 | doi = 10.1007/s00041-012-9242-5
 | arxiv = 1112.5469
 | bibcode = 2013JFAA...19..167G
 | s2cid = 1280745
 }}
* {{citation
 | last1 = Greiner | first1 = W.
 | last2 = Reinhardt | first2 = J.
 | title = Field Quantization
 | publisher = [[Springer-Verlag|Springer]]
 | year = 1996
 | isbn = 978-3-540-59179-5
 | url-access = registration
 | url = https://archive.org/details/fieldquantizatio0000grei
}}
* {{citation
 | last1 = Gelfand | first1 = I.M. | author1-link = Israel Gelfand
 | last2 = Shilov | first2 = G.E. | author2-link = Naum Ya. Vilenkin
 | title = Generalized Functions
 | volume = 1
 | publisher = [[Academic Press]]
 | location = New York
 | year = 1964
}} (translated from Russian)
* {{citation
 | last1 = Gelfand | first1 = I.M. | author1-link = Israel Gelfand
 | last2 = Shilov | first2 = G.E. | author2-link = Naum Ya. Vilenkin
 | title = Generalized Functions
 | volume = 2
 | publisher = [[Academic Press]]
 | location = New York
 | year = 1968
}} (translated from Russian)
* {{citation
 | last1 = Gelfand | first1 = I.M. | author1-link = Israel Gelfand
 | last2 = Vilenkin | first2 = N.Y. | author2-link = Naum Ya. Vilenkin
 | title = Generalized Functions
 | volume = 4
 | publisher = [[Academic Press]]
 | location = New York
 | year = 1964
}} (translated from Russian)
* {{citation
 | last1 = Hewitt | first1 = Edwin
 | last2 = Ross | first2 = Kenneth A.
 | title = Abstract harmonic analysis: Structure and analysis for compact groups. Analysis on locally compact Abelian groups
 | volume = II
 | publisher = [[Springer-Verlag|Springer]]
 | series = Die Grundlehren der mathematischen Wissenschaften, Band 152
 | mr = 0262773
 | year = 1970
}}
* {{citation
 | last = Hörmander | first = L. | author-link = Lars Hörmander
 | title = Linear Partial Differential Operators
 | volume = 1
 | publisher = [[Springer-Verlag|Springer]]
 | year = 1976
 | isbn = 978-3-540-00662-6
}}
* {{citation
 | last = Howe | first = Roger
 | title = On the role of the Heisenberg group in harmonic analysis
 | journal = [[Bulletin of the American Mathematical Society]]
 | volume = 3
 | pages = 821–844
 | number = 2
 | year = 1980
 | doi = 10.1090/S0273-0979-1980-14825-9
 | mr = 578375
 | doi-access = free
 }}
* {{citation
 | last = Hunter | first = J.K. 
 | title = Appendix: The Fourier transform
 | work = Lecture Notes on PDEs
 | url = https://www.math.ucdavis.edu/~hunter/pdes/pdes.html
 | access-date = January 12, 2025
 | year = 2014
}}
* {{citation
 | last = James | first = J.F.
 | title = A Student's Guide to Fourier Transforms
 | edition = 3rd
 | publisher = [[Cambridge University Press]]
 | year = 2011
 | bibcode = 2011sgft.book.....J
 | isbn = 978-0-521-17683-5
}}
* {{citation
 | last = Jordan | first = Camille | author-link = Camille Jordan
 | title = Cours d'Analyse de l'École Polytechnique
 | volume = II, Calcul Intégral: Intégrales définies et indéfinies
 | edition = 2nd
 | location = Paris
 | year = 1883
}}
* {{citation
 | last = Kaiser | first = Gerald
 | chapter = A Friendly Guide to Wavelets
 | title = Physics Today
 | volume = 48
 | issue = 7
 | pages = 57–58
 | year = 1994
 | isbn = 978-0-8176-3711-8
 | chapter-url = https://books.google.com/books?id=rfRnrhJwoloC&q=%22becomes+the+Fourier+%28integral%29+transform%22&pg=PA29
 | bibcode = 1995PhT....48g..57K
 | doi = 10.1063/1.2808105
 | chapter-url-access = subscription
 }}
* {{citation
 | last = Kammler | first = David
 | title = A First Course in Fourier Analysis
 | year = 2000
 | publisher = Prentice Hall
 | isbn = 978-0-13-578782-3
}}
* {{citation | last=Katznelson | first=Yitzhak | title=An Introduction to Harmonic Analysis | publisher=Cambridge University Press | date=2004 | isbn=978-0-521-83829-0 | doi=10.1017/cbo9781139165372 | url=https://www.cambridge.org/core/product/identifier/9781139165372/type/book| url-access=subscription }}
* {{citation
 | last1 = Khare | first1 = Kedar
 | last2 = Butola | first2 = Mansi
 | last3 = Rajora | first3 = Sunaina
 | title = Fourier Optics and Computational Imaging
 | publisher = Springer
 | year = 2023
 | isbn = 978-3-031-18353-9
 | edition = 2nd
 | chapter = Chapter 2.3 Fourier Transform as a Limiting Case of Fourier Series
 | doi = 10.1007/978-3-031-18353-9
 | s2cid = 255676773
 | doi-access = free
 }}
* {{citation
 | last1 = Kirillov | first1 = Alexandre | author1-link = Alexandre Kirillov
 | last2 = Gvishiani | first2 = Alexei D.
 | title = Theorems and Problems in Functional Analysis
 | year = 1982
 | orig-date = 1979
 | publisher = [[Springer-Verlag|Springer]]
}} (translated from Russian)
* {{citation
 | last = Knapp | first = Anthony W.
 | title = Representation Theory of Semisimple Groups: An Overview Based on Examples
 | url = https://books.google.com/books?id=QCcW1h835pwC
 | publisher = [[Princeton University Press]]
 | year = 2001
 | isbn = 978-0-691-09089-4
}}
* {{citation
 | last1 = Kolmogorov | first1 = Andrey Nikolaevich | author1-link = Andrey Kolmogorov
 | last2 = Fomin | first2 = Sergei Vasilyevich
 | author2-link = Sergei Fomin
 | title = Elements of the Theory of Functions and Functional Analysis
 | year = 1999
 | orig-date = 1957
 | publisher = [[Dover Publications|Dover]]
 | url = http://store.doverpublications.com/0486406830.html
}} (translated from Russian)
* {{citation
 | last = Lado | first = F.
 | title = Numerical Fourier transforms in one, two, and three dimensions for liquid state calculations
 | journal = [[Journal of Computational Physics]]
 | volume = 8
 | issue = 3
 | year = 1971
 | pages = 417–433
 | doi = 10.1016/0021-9991(71)90021-0
 | bibcode = 1971JCoPh...8..417L
 | url = https://www.lib.ncsu.edu/resolver/1840.2/2465
 | url-access = subscription
 }}
* {{cite journal | last=Lax | first=Peter D. | title=Integrals of nonlinear equations of evolution and solitary waves | journal=Communications on Pure and Applied Mathematics | volume=21 | issue=5 | date=1968 | issn=0010-3640 | doi=10.1002/cpa.3160210503 | doi-access=free | pages=467–490 | url=https://www.osti.gov/biblio/4522657 | access-date=2025-09-21}}
* {{citation| last=Mallat | first=Stéphane | author-link=Stephane Mallat| title=A wavelet tour of signal processing: the sparse way | publisher=Elsevier/Academic Press | publication-place=Amsterdam Boston | date=2009 | doi=10.1016/B978-0-12-374370-1.X0001-8|isbn=978-0-12-374370-1}}
* {{cite book | last1=Lieb | first1=Elliott H. | last2=Loss | first2=Michael | title=Analysis | publisher=American Mathematical Soc. | publication-place=Providence (R. I.) | date=2001 | isbn=0-8218-2783-9}}
* {{citation
 | last = Müller | first = Meinard
 | title = The Fourier Transform in a Nutshell.
 | url = https://www.audiolabs-erlangen.de/content/05-fau/professor/00-mueller/04-bookFMP/2015_Mueller_FundamentalsMusicProcessing_Springer_Section2-1_SamplePages.pdf
 | publisher = [[Springer-Verlag|Springer]]
 | year = 2015
 | doi = 10.1007/978-3-319-21945-5
 | isbn = 978-3-319-21944-8
 | s2cid = 8691186
 | access-date = 2016-03-28
 | archive-date = 2016-04-08
 | archive-url = https://web.archive.org/web/20160408083515/https://www.audiolabs-erlangen.de/content/05-fau/professor/00-mueller/04-bookFMP/2015_Mueller_FundamentalsMusicProcessing_Springer_Section2-1_SamplePages.pdf
 }}; also available at [http://www.music-processing.de Fundamentals of Music Processing], Section 2.1, pages 40–56
* {{citation
 |last1=Oppenheim |first1=Alan V. |author1-link=Alan V. Oppenheim
 |last2=Schafer |first2=Ronald W. |author2-link=Ronald W. Schafer
 |last3=Buck |first3=John R.
 |title=Discrete-time signal processing
 |year=1999
 |publisher=Prentice Hall
 |location=Upper Saddle River, N.J.
 |isbn=0-13-754920-2
 |edition=2nd
 |url-access=registration
 |url=https://archive.org/details/discretetimesign00alan
 }}
* {{citation
 | last1 = Paley | first1 = R.E.A.C. | author1-link = Raymond Paley
 | last2 = Wiener | first2 = Norbert | author2-link = Norbert Wiener
 | title = Fourier Transforms in the Complex Domain
 | series = American Mathematical Society Colloquium Publications
 | number = 19
 | year = 1934
 | publisher = [[American Mathematical Society]]
 | location = Providence, Rhode Island
}}
* {{citation
 | last = Pinsky | first = Mark
 | title = Introduction to Fourier Analysis and Wavelets
 | year = 2002
 | publisher = Brooks/Cole
 | isbn = 978-0-534-37660-4
 | url = https://books.google.com/books?id=PyISCgAAQBAJ&q=%22The+Fourier+transform+of+the+measure%22&pg=PA256
 }}
* {{citation
 | last = Poincaré | first = Henri | author-link = Henri Poincaré
 | title = Théorie analytique de la propagation de la chaleur
 | publisher = Carré
 | location = Paris
 | year = 1895
 | url = https://gallica.bnf.fr/ark:/12148/bpt6k5500702f
 }}
* {{citation
 | last1 = Polyanin | first1 = A. D.
 | last2 = Manzhirov | first2 = A. V.
 | title = Handbook of Integral Equations
 | publisher = [[CRC Press]]
 | location = Boca Raton
 | year = 1998
 | isbn = 978-0-8493-2876-3
}}
* {{citation
 | last1 = Press | first1 = William H.
 | last2 = Flannery | first2 = Brian P.
 | last3 = Teukolsky | first3 = Saul A.
 | last4 = Vetterling | first4 = William T.
 | title = Numerical Recipes in C: The Art of Scientific Computing, Second Edition
 | edition = 2nd
 | publisher = [[Cambridge University Press]]
 | year = 1992
}}
* {{cite book
 |last1 = Proakis |first1 = John G.
 |last2 = Manolakis |first2 = Dimitri G. |author2-link=Dimitris Manolakis
 |title = Digital Signal Processing: Principles, Algorithms and Applications
 |place = New Jersey
 |publisher = Prentice-Hall International
 |year = 1996
 |edition = 3rd
 |language = en
 |id = sAcfAQAAIAAJ
 |isbn = 978-0-13-373762-2
 |bibcode = 1996dspp.book.....P
 |url-access = registration
 |url = https://archive.org/details/digitalsignalpro00proa
 }}
* {{citation
 | last = Rahman | first = Matiur
 | url = https://books.google.com/books?id=k_rdcKaUdr4C&pg=PA10
 | isbn = 978-1-84564-564-9
 | publisher = WIT Press
 | title = Applications of Fourier Transforms to Generalized Functions
 | year = 2011
}}
* {{citation | last=Rudin | first=Walter | title=Fourier Analysis on Groups | publisher=John Wiley & Sons | publication-place=New York, NY | date=1991| isbn=978-0-471-52364-2}}
* {{citation
 | last = Rudin | first = Walter
 | title = Real and Complex Analysis
 | publisher = McGraw Hill
 | edition = 3rd
 | year = 1987
 | isbn = 978-0-07-100276-9
 | location = Singapore
}}
* {{citation
 | last1 = Simonen | first1 = P.
 | last2 = Olkkonen | first2 = H.
 | title = Fast method for computing the Fourier integral transform via Simpson's numerical integration
 | journal = Journal of Biomedical Engineering
 | volume = 7
 | issue = 4
 | year = 1985
 | pages = 337–340
 | doi=10.1016/0141-5425(85)90067-6
 | pmid = 4057997
}}
* {{cite web
 | last = Smith | first = Julius O.
 | url = https://ccrma.stanford.edu/~jos/mdft/Positive_Negative_Frequencies.html
 | title = Mathematics of the Discrete Fourier Transform (DFT), with Audio Applications --- Second Edition
 | website = ccrma.stanford.edu
 | access-date = 2022-12-29
 | quote = We may think of a real sinusoid as being the sum of a positive-frequency and a negative-frequency complex sinusoid.
 }}
* {{cite book | last=Stade | first=Eric | title=Fourier Analysis | publisher=Wiley | date=2005 | isbn=978-0-471-66984-5 | doi=10.1002/9781118165508}}
* {{citation
 | last1 = Stein | first1 = Elias
 | last2 = Shakarchi | first2 = Rami
 | title = Fourier Analysis: An introduction
 | publisher = [[Princeton University Press]]
 | year = 2003
 | isbn = 978-0-691-11384-5
 | url = https://books.google.com/books?id=FAOc24bTfGkC&q=%22The+mathematical+thrust+of+the+principle%22&pg=PA158
 }}
* {{citation
 | last1 = Stein | first1 = Elias | author1-link = Elias Stein
 | last2 = Weiss | first2 = Guido | author2-link = Guido Weiss
 | title = Introduction to Fourier Analysis on Euclidean Spaces
 | publisher = [[Princeton University Press]]
 | location = Princeton, N.J.
 | year = 1971
 | isbn = 978-0-691-08078-9
 | url = https://books.google.com/books?id=YUCV678MNAIC&q=editions:xbArf-TFDSEC
}}
* {{citation| last=Strichartz | first=Robert S. | author-link=Robert Strichartz| title=A guide to distribution theory and Fourier transforms | publisher=CRC Press | publication-place=Boca Raton | date=1994 | isbn=0-8493-8273-4}}
* {{citation
 | last = Taneja | first = H.C.
 | title = Advanced Engineering Mathematics
 | volume = 2
 | chapter-url = https://books.google.com/books?id=X-RFRHxMzvYC&q=%22The+Fourier+integral+can+be+regarded+as+an+extension+of+the+concept+of+Fourier+series%22&pg=PA192
 | chapter = Chapter 18: Fourier integrals and Fourier transforms
 | isbn = 978-81-89866-56-3
 | year = 2008
 | publisher = I. K. International Pvt Ltd
 | location = New Delhi, India
}}
* {{citation
 | last = Titchmarsh | first = E. | author-link = Edward Charles Titchmarsh
 | title = Introduction to the theory of Fourier integrals
 | isbn = 978-0-8284-0324-5
 | orig-date = 1948
 | year = 1986
 | edition = 2nd
 | publisher = [[Clarendon Press]]
 | location = Oxford University
}}
* {{citation
 | last = Vretblad | first = Anders
 | title = Fourier Analysis and its Applications
 | year = 2000
 | isbn = 978-0-387-00836-3
 | publisher = [[Springer-Verlag|Springer]]
 | series = [[Graduate Texts in Mathematics]]
 | volume = 223
 | location = New York
}}
* {{citation
 | last1 = Whittaker | first1 = E. T. | author1-link = E. T. Whittaker
 | last2 = Watson | first2 = G. N. | author2-link = G. N. Watson
 | title = A Course of Modern Analysis
 | title-link = A Course of Modern Analysis
 | edition = 4th
 | publisher = [[Cambridge University Press]]
 | year = 1927
}}
* {{citation
 | last1 = Widder | first1 = David Vernon
 | last2 = Wiener | first2 = Norbert | author2-link = Norbert Wiener
 | title = Remarks on the Classical Inversion Formula for the Laplace Integral
 | date = August 1938
 | journal = Bulletin of the American Mathematical Society
 | volume = 44
 | issue = 8
 | pages = 573–575
 | doi = 10.1090/s0002-9904-1938-06812-7
 | url = https://projecteuclid.org/euclid.bams/1183500627
 | doi-access = free
}}
* {{cite book |last=Wiener |first=Norbert |author-link=Norbert Wiener |year=1949 |title=Extrapolation, Interpolation, and Smoothing of Stationary Time Series: With Engineering Applications |url=https://direct.mit.edu/books/oa-monograph/4361/Extrapolation-Interpolation-and-Smoothing-of |publisher=[[MIT Press]] |isbn=978-0-262-25719-0 }}
* {{citation
 | last = Wilson | first = R. G.
 | title = Fourier Series and Optical Transform Techniques in Contemporary Optics
 | publisher = [[John Wiley & Sons|Wiley]]
 | year = 1995
 | isbn = 978-0-471-30357-2
 | location = New York
}}
* {{citation
 | last = Wolf | first = Kurt B.
 | title = Integral Transforms in Science and Engineering
 | publisher = [[Springer-Verlag|Springer]]
 | year = 1979
 | doi = 10.1007/978-1-4757-0872-1
 | isbn = 978-1-4757-0874-5
 | url = https://www.fis.unam.mx/~bwolf/integraleng.html
 | url-access = subscription
}}
* {{citation
 | last = Yosida | first = K. | author-link = Kōsaku Yosida
 | title = Functional Analysis
 | publisher = [[Springer-Verlag|Springer]]
 | year = 1968
 | isbn = 978-3-540-58654-8
}}
* {{cite journal | last1=Yousefi | first1=Mansoor I | last2=Kschischang | first2=Frank R | title=Information Transmission Using the Nonlinear Fourier Transform, Part I: Mathematical Tools | journal=IEEE Transactions on Information Theory | volume=60 | issue=7 | date=2014 | issn=0018-9448 | doi=10.1109/TIT.2014.2321143 | doi-access=free | pages=4312–4328 | url=http://arxiv.org/pdf/1202.3653 | access-date=2025-09-21| arxiv=1202.3653 }}
{{refend}}

== External links ==
* {{Commons category-inline}}
* [https://www.encyclopediaofmath.org/index.php/Fourier_transform Encyclopedia of Mathematics]
* {{MathWorld | urlname = FourierTransform | title = Fourier Transform}}
* [https://www.xtal.iqf.csic.es/Cristalografia/parte_05-en.html Fourier Transform in Crystallography]

{{Authority control}}

{{DEFAULTSORT:Fourier Transform}}
[[Category:Fourier analysis]]
[[Category:Integral transforms]]
[[Category:Unitary operators]]
[[Category:Joseph Fourier]]
[[Category:Mathematical physics]]