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<record version="12" id="5611">
 <title>topics in manifold theory</title>
 <name>Manifold2</name>
 <created>2004-02-22 04:23:33</created>
 <modified>2007-12-12 12:51:55</modified>
 <type>Topic</type>
 <creator id="5830" name="evin290"/>
 <author id="4157" name="jirka"/>
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 <author id="12619" name="juanman"/>
 <author id="146" name="rmilson"/>
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 <author id="4804" name="Grayum"/>
 <author id="1858" name="matte"/>
 <classification>
	<category scheme="msc" code="53-00"/>
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 <content>A {\em manifold} is a space that is
locally like $\mathbb{R}^n$, however lacking a preferred system of
coordinates. Furthermore, a manifold can have global topological
properties, such as non-contractible \PMlinkname{loops}{Curve}, that distinguish it from
the topologically trivial $\mathbb{R}^n$.
 

By imposing different restrictions on the transition functions of a manifold, one
obtain different types of manifolds:
\begin{itemize}
\item topological manifolds
\item $C^k$ manifolds, smooth manifolds
\item real analytic manifold
\item complex analytic manifold
\item symplectic manifolds, where transition functions
are symplectomorphisms. On such manifolds,  one can formulate the 
Hamilton equations. 
\end{itemize}

Special types of manifolds
\begin{itemize}
\item orientable manifolds
\item manifolds with boundary
\item compact manifolds
\end{itemize}

On manifolds, one can introduce more \PMlinkescapetext{structure}. Some examples are:
\begin{itemize}
\item Riemannian manifolds
\item contact manifolds
\item CR manifolds
\item fiber bundles and sheaves
\end{itemize}

\subsubsection*{Examples}
\begin{itemize}
\item space-time manifold in general relativity
\item phase space in mechanics
\item de Rham cohomology in algebraic topology
\end{itemize}

\subsubsection*{See also}
For the formal definition click \PMlinkname{here}{Manifold}\\
\PMlinkexternal{Manifold entry at Wikipedia}{http://en.wikipedia.org/wiki/Manifold}</content>
</record>
