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

<record version="8" id="3667">
 <title>symplectic manifold</title>
 <name>SymplecticManifold</name>
 <created>2002-12-05 23:30:37</created>
 <modified>2006-07-09 12:21:59</modified>
 <type>Definition</type>
 <creator id="1858" name="matte"/>
 <author id="13753" name="Mathprof"/>
 <author id="1858" name="matte"/>
 <author id="988" name="bwebste"/>
 <classification>
	<category scheme="msc" code="53D05"/>
 </classification>
 <defines>
	<concept>symplectic form</concept>
	<concept>symplectomorphism</concept>
	<concept>canonical transformation</concept>
 </defines>
 <related>
	<object name="ContactManifold"/>
	<object name="KahlerManifold"/>
	<object name="HyperkahlerManifold"/>
	<object name="MathbbCIsAKahlerManifold"/>
 </related>
 <preamble>% this is the default PlanetMath preamble.  as your knowledge
% of TeX increases, you will probably want to edit this, but
% it should be fine as is for beginners.

% almost certainly you want these
\usepackage{amssymb}
\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{amsthm}

\usepackage{mathrsfs}

% used for TeXing text within eps files
%\usepackage{psfrag}
% need this for including graphics (\includegraphics)
%\usepackage{graphicx}
% for neatly defining theorems and propositions
%
% making logically defined graphics
%\usepackage{xypic}

% there are many more packages, add them here as you need them

% define commands here

\newcommand{\sR}[0]{\mathbb{R}}
\newcommand{\sC}[0]{\mathbb{C}}
\newcommand{\sN}[0]{\mathbb{N}}
\newcommand{\sZ}[0]{\mathbb{Z}}

 \usepackage{bbm}
 \newcommand{\Z}{\mathbbmss{Z}}
 \newcommand{\C}{\mathbbmss{C}}
 \newcommand{\R}{\mathbbmss{R}}
 \newcommand{\Q}{\mathbbmss{Q}}



\newcommand*{\norm}[1]{\lVert #1 \rVert}
\newcommand*{\abs}[1]{| #1 |}



\newtheorem{thm}{Theorem}
\newtheorem{defn}{Definition}
\newtheorem{prop}{Proposition}
\newtheorem{lemma}{Lemma}
\newtheorem{cor}{Corollary}</preamble>
 <content>Symplectic manifolds constitute
the mathematical structure for modern Hamiltonian mechanics.
Symplectic manifolds can also be seen as even dimensional 
analogues to contact manifolds. 

\begin{defn}
A {\em symplectic manifold} is a pair $(M,\omega)$ consisting 
of a smooth manifold $M$ and a 
closed \PMlinkname{2-form}{DifferentialForms} 
$\omega\in\Omega^2(M)$, that is non-degenerate
at each point.  
Then $\omega$ is called a {\em symplectic 
form} for $M$.
\end{defn}

\subsubsection*{Properties}
\begin{enumerate}
\item Every symplectic manifold is even dimensional. This is 
easy to understand in view of the physics. In Hamilton
equations, location and momentum vectors always appear in pairs.
\item A form $\omega\in \Omega^2(M)$ on a $2n$-dimensional 
manifold $M$ is non-degenerate if and only if the 
$n$-fold product $\omega^n= \omega\wedge \cdots \wedge \omega$
is non-zero.
\item As a consequence of the last \PMlinkescapetext{property}, every symplectic manifold
is orientable. 
\end{enumerate}

Let $(M,\omega)$ and $(N,\eta)$ be symplectic manifolds.  Then a diffeomorphism $f\colon M\to N$ is
called a {\em symplectomorphism} if $f^*\eta=\omega$, that is, if the symplectic form on $N$
pulls back to the form on $M$.

\subsubsection*{Notes}
A symplectomorphism is also known as a \emph{canonical transformation}.
This \PMlinkescapetext{term} is mostly used in the mechanics literature.</content>
</record>
