<?xml version="1.0" encoding="UTF-8"?>

<record version="5" id="685">
 <title>table of  Fourier and generalized transforms</title>
 <name>TableOfFourierAndGeneralizedTransforms</name>
 <created>2009-04-22 11:40:14</created>
 <modified>2009-04-22 11:49:58</modified>
 <type>Data Structure</type>
 <creator id="441" name="bci1"/>
 <modifier id="441" name="bci1"/>
 <author id="441" name="bci1"/>
 <classification>
	<category scheme="msc" code="00."/>
	<category scheme="msc" code="02."/>
 </classification>
 <keywords>
	<term>Fourier transform</term>
	<term>Fourier-Stieltjes transform</term>
	<term>Radon transform</term>
	<term>Laplace transform</term>
 </keywords>
 <preamble>% almost certainly you want these
\usepackage{amssymb}
\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{tabls}

% define commands here
\usepackage{amsmath, amssymb, amsfonts, amsthm, amscd, latexsym, enumerate}
\usepackage{xypic, xspace}
\usepackage[mathscr]{eucal}
\usepackage[dvips]{graphicx}
\usepackage[curve]{xy}
\theoremstyle{plain}
\newtheorem{lemma}{Lemma}[section]
\newtheorem{proposition}{Proposition}[section]
\newtheorem{theorem}{Theorem}[section]
\newtheorem{corollary}{Corollary}[section]
\theoremstyle{definition}
\newtheorem{definition}{Definition}[section]
\newtheorem{example}{Example}[section]
%\theoremstyle{remark}
\newtheorem{remark}{Remark}[section]
\newtheorem*{notation}{Notation}
\newtheorem*{claim}{Claim}
\renewcommand{\thefootnote}{\ensuremath{\fnsymbol{footnote}}}
\numberwithin{equation}{section}
\newcommand{\Ad}{{\rm Ad}}
\newcommand{\Aut}{{\rm Aut}}
\newcommand{\Cl}{{\rm Cl}}
\newcommand{\Co}{{\rm Co}}
\newcommand{\DES}{{\rm DES}}
\newcommand{\Diff}{{\rm Diff}}
\newcommand{\Dom}{{\rm Dom}}
\newcommand{\Hol}{{\rm Hol}}
\newcommand{\Mon}{{\rm Mon}}
\newcommand{\Hom}{{\rm Hom}}
\newcommand{\Ker}{{\rm Ker}}
\newcommand{\Ind}{{\rm Ind}}
\newcommand{\IM}{{\rm Im}}
\newcommand{\Is}{{\rm Is}}
\newcommand{\ID}{{\rm id}}
\newcommand{\grpL}{{\rm GL}}
\newcommand{\Iso}{{\rm Iso}}
\newcommand{\rO}{{\rm O}}
\newcommand{\Sem}{{\rm Sem}}
\newcommand{\SL}{{\rm Sl}}
\newcommand{\St}{{\rm St}}
\newcommand{\Sym}{{\rm Sym}}
\newcommand{\Symb}{{\rm Symb}}
\newcommand{\SU}{{\rm SU}}
\newcommand{\Tor}{{\rm Tor}}
\newcommand{\U}{{\rm U}}
\newcommand{\A}{\mathcal A}
\newcommand{\Ce}{\mathcal C}
\newcommand{\D}{\mathcal D}
\newcommand{\E}{\mathcal E}
\newcommand{\F}{\mathcal F}
%\newcommand{\grp}{\mathcal G}
\renewcommand{\H}{\mathcal H}
\renewcommand{\cL}{\mathcal L}
\newcommand{\Q}{\mathcal Q}
\newcommand{\R}{\mathcal R}
\newcommand{\cS}{\mathcal S}
\newcommand{\cU}{\mathcal U}
\newcommand{\W}{\mathcal W}
\newcommand{\bA}{\mathbb{A}}
\newcommand{\bB}{\mathbb{B}}
\newcommand{\bC}{\mathbb{C}}
\newcommand{\bD}{\mathbb{D}}
\newcommand{\bE}{\mathbb{E}}
\newcommand{\bF}{\mathbb{F}}
\newcommand{\bG}{\mathbb{G}}
\newcommand{\bK}{\mathbb{K}}
\newcommand{\bM}{\mathbb{M}}
\newcommand{\bN}{\mathbb{N}}
\newcommand{\bO}{\mathbb{O}}
\newcommand{\bP}{\mathbb{P}}
\newcommand{\bR}{\mathbb{R}}
\newcommand{\bV}{\mathbb{V}}
\newcommand{\bZ}{\mathbb{Z}}
\newcommand{\bfE}{\mathbf{E}}
\newcommand{\bfX}{\mathbf{X}}
\newcommand{\bfY}{\mathbf{Y}}
\newcommand{\bfZ}{\mathbf{Z}}
\renewcommand{\O}{\Omega}
\renewcommand{\o}{\omega}
\newcommand{\vp}{\varphi}
\newcommand{\vep}{\varepsilon}
\newcommand{\diag}{{\rm diag}}
\newcommand{\grp}{\mathcal G}
\newcommand{\dgrp}{{\mathsf{D}}}
\newcommand{\desp}{{\mathsf{D}^{\rm{es}}}}
\newcommand{\grpeod}{{\rm Geod}}
%\newcommand{\grpeod}{{\rm geod}}
\newcommand{\hgr}{{\mathsf{H}}}
\newcommand{\mgr}{{\mathsf{M}}}
\newcommand{\ob}{{\rm Ob}}
\newcommand{\obg}{{\rm Ob(\mathsf{G)}}}
\newcommand{\obgp}{{\rm Ob(\mathsf{G}')}}
\newcommand{\obh}{{\rm Ob(\mathsf{H})}}
\newcommand{\Osmooth}{{\Omega^{\infty}(X,*)}}
\newcommand{\grphomotop}{{\rho_2^{\square}}}
\newcommand{\grpcalp}{{\mathsf{G}(\mathcal P)}}
\newcommand{\rf}{{R_{\mathcal F}}}
\newcommand{\grplob}{{\rm glob}}
\newcommand{\loc}{{\rm loc}}
\newcommand{\TOP}{{\rm TOP}}
\newcommand{\wti}{\widetilde}
\newcommand{\what}{\widehat}
\renewcommand{\a}{\alpha}
\newcommand{\be}{\beta}
\newcommand{\grpa}{\grpamma}
%\newcommand{\grpa}{\grpamma}
\newcommand{\de}{\delta}
\newcommand{\del}{\partial}
\newcommand{\ka}{\kappa}
\newcommand{\si}{\sigma}
\newcommand{\ta}{\tau}
\newcommand{\lra}{{\longrightarrow}}
\newcommand{\ra}{{\rightarrow}}
\newcommand{\rat}{{\rightarrowtail}}
\newcommand{\ovset}[1]{\overset {#1}{\ra}}
\newcommand{\ovsetl}[1]{\overset {#1}{\lra}}
\newcommand{\hr}{{\hookrightarrow}}

\newcommand{\&lt;}{{\langle}}

%\newcommand{\&gt;}{{\rangle}}

\def\baselinestretch{1.1}
\hyphenation{prod-ucts}

%\grpeometry{textwidth= 16 cm, textheight=21 cm}

\newcommand{\sqdiagram}[9]{$$ \diagram #1 \rto^{#2} \dto_{#4}&amp;
#3 \dto^{#5} \\ #6 \rto_{#7} &amp; #8 \enddiagram
\eqno{\mbox{#9}}$$ }
\def\C{C^{\ast}}
\newcommand{\labto}[1]{\stackrel{#1}{\longrightarrow}}

%\newenvironment{proof}{\noindent {\bf Proof} }{ \hfill $\Box$
%{\mbox{}}
\newcommand{\quadr}[4]
{\begin{pmatrix} &amp; #1&amp; \\[-1.1ex] #2 &amp; &amp; #3\\[-1.1ex]&amp; #4&amp;
\end{pmatrix}}
\def\D{\mathsf{D}}</preamble>
 <content>\subsection{Table of Fourier and generalized transforms}

\textbf{Fourier-Stieltjes} transforms and \textbf{measured groupoid} transforms are useful generalizations of the (much simpler) Fourier transform, as concisely shown in the following table.


\subsubsection*{FT and FT Generalized Transforms}
\begin{center}
\begin{tabular}{|c|c|c|c|c|}
\hline\hline
$f(t)$ &amp; $\F{f(t)} = \hat{f}(x)$ &amp; Conditions* &amp; Explanation &amp; Description \\
\hline
$c$ &amp; $(\sqrt{2 \pi})^{-1}c$ &amp; Notice on the next line the overline bar placed above $t(x)$  &amp; &amp;\\
&amp; &amp; \\ &amp; &amp; \\
\hline
Gaussian function &amp; Gaussian function &amp; \\&amp; &amp;\\
&amp; &amp; \\ &amp; &amp; \\
\hline
Lorentzian function &amp; Lorentzian function &amp; \\&amp; &amp;\\
&amp; &amp; \\ &amp; &amp; \\
\hline
step function &amp; $Sin(x)/x$ &amp; \\&amp; &amp; \\
&amp; &amp; \\ &amp; &amp; \\
\hline
sawtooth function &amp; $Sin^2(x)/x^2$ &amp; \\&amp; &amp; \\
&amp; &amp; \\ &amp; &amp; \\
\hline
$f(t)$ &amp; $\int \hat{f}(x) \overline{t(x)}dx$ &amp; $f(t)\in{L^1(G_l)}$, with $G_l$ a &amp; Fourier-Stieltjes transform &amp; $\hat{f}(x)\in{C_0(\hat{G_l})}$ \\
&amp; &amp; locally compact groupoid \cite{RW97}; &amp; &amp; \\
&amp; &amp; $\int $ is defined \emph{via} &amp; &amp; \\
&amp; &amp; a left Haar measure on $G_l$ &amp; &amp; \\
\hline
$\hat{m}(x)$ &amp; $\check{m}(t)= \int e^{itx}d\hat{m}(x)$ &amp; as above &amp; Inverse Fourier-Stieltjes &amp; $\check{m}(t) \in{L^1(G_l)}$, \\
&amp; &amp; &amp; transform &amp; (\cite{PALT2k1}, \cite{PALT2k3}). \\
\hline
$\hat{m}(x)$ &amp; $\check{m}(t) = \int e^{itx}d\hat{m}(x)$ &amp; When $G_l=\mathbb{R}$, and it exists &amp; This is the usual &amp; $\check{m}(t) \in{\mathbb{R}}$ \\
&amp; &amp; only when $\hat{m}(x)$ is &amp; Inverse Fourier transform &amp; \\
&amp; &amp; \emph{Lebesgue integrable} on &amp; &amp; \\
&amp; &amp; the entire real axis &amp; &amp; \\
\hline\hline


\end{tabular}
\end{center}
*Note the `slash hat' on $\hat{f}(x)$ and $\hat{G_l}$.

\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>
</record>
