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<record version="7" id="7688">
 <title>pseudo-Riemannian manifold</title>
 <name>PseudoRiemannianManifold</name>
 <created>2006-03-06 16:08:31</created>
 <modified>2007-08-07 18:47:17</modified>
 <type>Definition</type>
 <creator id="11260" name="cvalente"/>
 <author id="11260" name="cvalente"/>
 <classification>
	<category scheme="msc" code="53Z05"/>
 </classification>
 <defines>
	<concept>pseudo-Riemannian geometry</concept>
	<concept>pseudo-Riemannian manifold</concept>
 </defines>
 <related>
	<object name="EinsteinFieldEquations"/>
	<object name="SylvestersLaw"/>
	<object name="MinkowskiSpace"/>
	<object name="CategoryOfRiemannianManifolds"/>
 </related>
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 <content>A \emph{pseudo-Riemannian} manifold is a manifold $M$ together with a \PMlinkname{non degenerate}{NonDegenerateBilinearForm}, symmetric section $g$ of $T^0_{2}(M)$ (2-covariant tensor bundle over $M$).

Unlike with a Riemannian manifold, $g$ is not positive definite. That is, there exist vectors $v\in T_{p}M$ such that $g(v,v)\le0$.

A well known \PMlinkname{result from linear algebra}{SylvestersLaw} permits us to make a change of basis such that in the new base $g$ is represented by a diagonal matrix with $-1$ or $1$ elements in the diagonal. If there are $i$, $-1$ elements in the diagonal and $j$, $1$, the tensor is said to have signature $(i,j)$

The signature will be invariant in every connected component of $M$, but usually the restriction that it be a global invariant is added to the definition of a pseudo-Riemannian manifold.

Unlike a Riemannian metric, some manifolds do not admit a pseudo-Riemannian metric.

Pseudo-Riemannian manifolds are crucial in Physics and in particular in General Relativity where space-time is modeled as a 4-pseudo Riemannian manifold with signature (1,3)\footnote{also referred to as $(-+++)$}.

Intuitively pseudo-Riemannian manifolds are generalizations of Minkowski's space just as a Riemannian manifold is a generalization of a vector space with a positive definite metric.</content>
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