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 <title>table of  Fourier and generalized transforms</title>
 <name>TableOfFourierAndGeneralizedTransforms</name>
 <created>2009-04-22 11:40:14</created>
 <modified>2026-09-09 21:46:29</modified>
 <type>Data Structure</type>
 <creator id="441" name="bci1"/>
 <modifier id="1" name="bloftin"/>
 <comment>section numbering</comment>
 <author id="441" name="bci1"/>
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	<category scheme="pacs" code="02."/>
 </classification>
 <defines>
	<concept>quantum theories on a lattice</concept>
	<concept>QM</concept>
	<concept>QTL</concept>
	<concept>FT-NIR</concept>
	<concept>FT-IR</concept>
 </defines>
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	<synonym concept="table of  Fourier and generalized transforms" alias="FT"/>
	<synonym concept="table of  Fourier and generalized transforms" alias="FFT"/>
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	<object name="TableOfLaplaceTransforms"/>
	<object name="BesselFunctionsAndTheirApplicationsToDiffractionByHelicalStructures"/>
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 <keywords>
	<term>Fourier transform</term>
	<term>Fourier-Stieltjes transform</term>
	<term>table of Fourier and generalized transforms</term>
	<term>Radon transform</term>
	<term>Laplace transform</term>
	<term>FT-NIR</term>
	<term>FT-IR</term>
	<term>QCD</term>
	<term>QG</term>
	<term>QFT</term>
	<term>QLT</term>
	<term>AQFT</term>
	<term>quantum theories on a lattice</term>
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 <content>\subsection{Table of Fourier and Generalized Fourier Transforms}

Fourier transforms are widely employed in physical, chemical, and engineering
applications for harmonic analysis and for processing acquired data, such as
spectroscopic data and images. Applications include astrophysics, electron
microscopy, optics, structure determination (for example, X-ray, neutron, and
electron diffraction), chemical hyperspectral imaging (FT-NIR and FT-IR), and
many others. Theoretical studies in quantum mechanics (QM), QCD, QG, AQFT, and
quantum theories on a lattice (QTL) also employ Fourier transforms.

\textbf{Fourier--Stieltjes transforms} and \textbf{measured groupoid transforms}
are useful generalizations of the ordinary Fourier transform, as summarized in
the following table.

\subsubsection*{Fourier Transforms and Generalized FTs}

\begin{center}
\begin{tabular}{|p{0.16\textwidth}|p{0.20\textwidth}|p{0.20\textwidth}|p{0.18\textwidth}|p{0.18\textwidth}|}
\hline
$f(t)$ &amp;
$\mathcal{F}\{f(t)\}=\hat{f}(x)$ &amp;
Conditions &amp;
Explanation &amp;
Description
\tabularnewline
\hline

Gaussian function &amp;
Gaussian function &amp;
general &amp;
In statistics and spectroscopy &amp;
Gaussian profiles remain Gaussian under Fourier transformation
\tabularnewline
\hline

Lorentzian function &amp;
Exponential-type transform &amp;
general &amp;
In spectroscopy &amp;
Associated with exponentially decaying time-domain signals
\tabularnewline
\hline

Step or rectangular function &amp;
$\sin(x)/x$-type function &amp;
general &amp;
FT of a rectangular pulse &amp;
Sinc-type transform
\tabularnewline
\hline

Triangular function &amp;
$\sin^2(x)/x^2$-type function &amp;
general &amp;
Transform of a triangular profile &amp;
Squared-sinc-type transform
\tabularnewline
\hline

Series of equidistant points &amp;
Periodic reciprocal-space series &amp;
general &amp;
Ideal periodic lattice &amp;
Used in diffraction theory
\tabularnewline
\hline

Lattice of infinite planes &amp;
Series of equidistant reciprocal-space points &amp;
general &amp;
One-dimensional reciprocal space &amp;
Used in crystallography and diffraction theory
\tabularnewline
\hline

Helix wrapped on a cylinder &amp;
Bessel functions or Bessel--Fourier series &amp;
general &amp;
Physical crystallography &amp;
Experimentally truncated to a finite number of Bessel terms
\tabularnewline
\hline

$c$ &amp;
$(\sqrt{2\pi})^{-1}c$ &amp;
Convention-dependent &amp;
Constant input &amp;
Normalization depends on Fourier-transform convention
\tabularnewline
\hline

$f(t)$ &amp;
$\displaystyle \int \hat{f}(x)\,\overline{t(x)}\,dx$ &amp;
$f(t)\in L^1(G_l)$, with $G_l$ a locally compact groupoid \cite{RW97};
the integral is defined using a left Haar measure on $G_l$ &amp;
Fourier--Stieltjes transform &amp;
$\hat{f}(x)\in C_0(\widehat{G_l})$
\tabularnewline
\hline

$\hat{m}(x)$ &amp;
$\displaystyle \check{m}(t)=\int e^{itx}\,d\hat{m}(x)$ &amp;
as above &amp;
Inverse Fourier--Stieltjes transform &amp;
$\check{m}(t)\in L^1(G_l)$
(\cite{PALT2k1}, \cite{PALT2k3})
\tabularnewline
\hline

$\hat{m}(x)$ &amp;
$\displaystyle \check{m}(t)=\int e^{itx}\,d\hat{m}(x)$ &amp;
When $G_l=\mathbb{R}$ and the integral exists &amp;
Usual inverse Fourier transform &amp;
$\check{m}(t)\in\mathbb{R}$
\tabularnewline
\hline
\end{tabular}
\end{center}

\emph{Note.} The hat on $\hat{f}(x)$ and $\widehat{G_l}$ denotes the transformed
quantity or, in the latter case, the dual object.

\begin{thebibliography}{9}

\bibitem{RW97}
A. Ramsay and M. E. Walter,
Fourier--Stieltjes algebras of locally compact groupoids,
\emph{J. Functional Anal.} \textbf{148}: 314--367 (1997).

\bibitem{PALT2k1}
A. L. T. Paterson,
The Fourier algebra for locally compact groupoids,
Preprint (2001).

\bibitem{PALT2k3}
A. L. T. Paterson,
The Fourier--Stieltjes and Fourier algebras for locally compact groupoids
(2003).
\PMlinkexternal{Free PDF file download}{http://aux.planetmath.org/files/objects/10739/AFourierStjelties_LocallyCompactsGds_Harmonic0310138v1.pdf}

\end{thebibliography}
</content>
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