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\newcommand{\widevec}{\overrightarrow} \newcommand{\darr}{\downarrow} \newcommand{\nearr}{\nearrow} \newcommand{\nwarr}{\nwarrow} \newcommand{\searr}{\searrow} \newcommand{\swarr}{\swarrow} \newcommand{\curvearrowbotright}{\curvearrowright} \newcommand{\uparr}{\uparrow} \newcommand{\downuparrow}{\updownarrow} \newcommand{\duparr}{\updownarrow} \newcommand{\updarr}{\updownarrow} \newcommand{\gt}{>} \newcommand{\lt}{<} \newcommand{\map}{\mapsto} \newcommand{\embedsin}{\hookrightarrow} \newcommand{\Alpha}{A} \newcommand{\Beta}{B} \newcommand{\Zeta}{Z} \newcommand{\Eta}{H} \newcommand{\Iota}{I} \newcommand{\Kappa}{K} \newcommand{\Mu}{M} \newcommand{\Nu}{N} \newcommand{\Rho}{P} \newcommand{\Tau}{T} \newcommand{\Upsi}{\Upsilon} \newcommand{\omicron}{o} \newcommand{\lang}{\langle} \newcommand{\rang}{\rangle} \newcommand{\Union}{\bigcup} \newcommand{\Intersection}{\bigcap} \newcommand{\Oplus}{\bigoplus} \newcommand{\Otimes}{\bigotimes} \newcommand{\Wedge}{\bigwedge} \newcommand{\Vee}{\bigvee} 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\newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{Poisson summation formula} \hypertarget{idea}{}\subsection*{{Idea}}\label{idea} A certain identity for certain [[Fourier transforms]], equating a sum or integral of a function over a domain (e.g., a lattice) with a corresponding sum or integral of its Fourier dual over a dual domain (e.g., the dual lattice). \hypertarget{statement}{}\subsection*{{Statement}}\label{statement} The Poisson summation formula is basic to harmonic analysis over general locally compact Hausdorff abelian groups. Consider an exact sequence in $TopAb$ of [[locally compact space|locally compact]] [[Hausdorff space|Hausdorff]] [[topological abelian group|abelian groups]] \begin{displaymath} 0 \to A \to B \to C \to 0. \end{displaymath} where $A, B, C$ are equipped with Haar measures $d\mu_A, d\mu_B, d\mu_C$ that make the following equation true: \begin{displaymath} \int_B f(b)\; d\mu_B(b) = \int_C \int_A f(a + c)\; d\mu_A(a) d\mu_C(c) \end{displaymath} for all [[continuous functions]] $f: B \to \mathbb{C}$ with [[compact support]]. (The inner integral on the right is a shorthand for $\int_A f(a + b)\; d\mu_A(a)$ for any $b \in B$ that maps to $c \in C$; this is well-defined since the integral is invariant under changes $b \mapsto b + a'$ within the same coset $c$.) We remark that given Haar measures $d\mu_A, d\mu_B$, there exists a Haar measure $d\mu_C$ making this Fubini-type equation true. Then, since Haar measures form a torsor over the group of positive reals with multiplication, it follows that any two of $d\mu_A, d\mu_B, d\mu_C$ determine the third. In this notation, the ``Poisson summation formula'' is the equation asserted by the following result. \begin{theorem} \label{}\hypertarget{}{} Let $\widehat{C}$ denote the [[Pontryagin duality|Pontryagin dual]] of $C$, and $d\mu_{\widehat{C}}$ the dual Haar measure. For any [[Schwartz-Bruhat function]] $f: B \to \mathbb{C}$, we have \begin{displaymath} \int_A f(a)\; d\mu_A = \int_{\widehat{C}} \widehat{f}(\widehat{c})\; d\mu_{\widehat{C}} \end{displaymath} where $\widehat{f}$ is the Fourier dual of $f$, as a function on $\widehat{B}$. \end{theorem} In the special case of a [[lattice (discrete subgroup)|lattice]] $L$ inside $B$, the dual space $L^\perp = \widehat{B/L}$ is a lattice inside $\widehat{B}$, and the integrals are over discrete spaces, i.e. integration is just summation and we have \begin{displaymath} \sum_{x \in L} f(x) = \frac1{\mu(B/L)} \sum_{y \in L^\perp} \widehat{f}(y) \end{displaymath} where $\mu$ is the Haar measure on $B/L$ (as above). Often the measure on $B$ is chosen so that $\mu(B/L) = 1$. The classical case is when $B$ is a [[Euclidean space]] $\mathbb{R}^n$. But another case of a lattice inside locally compact abelian groups occurs in the context of \hyperlink{Tate1950}{Tate's thesis}, where a [[global field]] is viewed as a lattice inside its [[ring of adeles]]. \hypertarget{examples}{}\subsection*{{Examples}}\label{examples} \begin{itemize}% \item The Poisson summation formulation implies the [[functional equation]] for the [[Jacobi theta function]], which in turn implies that of the [[Riemann zeta function]], see at \emph{\href{Riemann+zeta+function#functional_equation}{Riemann zeta function -- functional identity}}. \end{itemize} \hypertarget{related_entries}{}\subsection*{{Related entries}}\label{related_entries} \begin{itemize}% \item [[functional equation]] \item A nonabelian version of the Poisson summation formula is the [[Selberg trace formula]]. \end{itemize} \hypertarget{references}{}\subsection*{{References}}\label{references} Reviews include \begin{itemize}% \item theorem 4.1 in \emph{Analytic theory of modular forms} \href{http://www.math.harvard.edu/~jbland/ma259x_notes.pdf}{pdf} \item E. Kowalski, prop. 2.2.1 in \emph{Automorphic forms, L-functions and number theory (March 12--16) Three Introductory lectures} (\href{http://www.math.ethz.ch/~kowalski/lectures.pdf}{pdf}) \end{itemize} An application to [[zeta functions]] via harmonic analysis on [[adele rings]] originates in Tate's thesis: \begin{itemize}% \item [[John Tate]], \emph{[[Fourier analysis in number fields, and Hecke's zeta-functions]]}, Princeton, May 1950, thesis; reproduced in \emph{Algebraic Number Theory} (Proc. Instructional Conf., Brighton, 1965) pp. 305--347, Academic Press 1967 \href{http://www.ams.org/mathscinet-getitem?mr=0217026}{MR0217026} \end{itemize} A textbook account is \begin{itemize}% \item [[Dorian Goldfeld]], [[Joseph Hundley]], chapter 2 of \emph{Automorphic representations and L-functions for the general linear group}, Cambridge Studies in Advanced Mathematics 129, 2011 (\href{https://www.maths.nottingham.ac.uk/personal/ibf/text/gl2.pdf}{pdf}) \end{itemize} and brief review in \begin{itemize}% \item [[Paul Garrett]], \emph{Iwasawa-Tate on $\zeta$-functions and L-functions}, 2011 (\href{http://www-users.math.umn.edu/~garrett/m/mfms/notes_c/Iwasawa-Tate.pdf}{pdf} [[!redirects Poisson formula]] \end{itemize} \end{document}