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		<summary type="html">&lt;p&gt;72.69.191.139: /* Gases */&lt;/p&gt;
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&lt;div&gt;In [[Riemannian geometry]], the &#039;&#039;&#039;sectional curvature&#039;&#039;&#039; is one of the ways to describe the [[curvature of Riemannian manifolds]]. The sectional curvature &#039;&#039;K&#039;&#039;(&amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt;) depends on a two-dimensional plane &amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt; in the tangent space at &#039;&#039;p&#039;&#039;. It is the [[Gaussian curvature]] of the [[surface]] which has the plane &amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt; as a tangent plane at &#039;&#039;p&#039;&#039;, obtained from [[geodesic]]s which start at &#039;&#039;p&#039;&#039; in the directions of &amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt; (in other words, the image of &amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt; under the [[exponential map]] at &#039;&#039;p&#039;&#039;). The sectional curvature is a smooth real-valued function on the 2-[[Grassmannian]] [[fiber bundle|bundle]] over the manifold.&lt;br /&gt;
&lt;br /&gt;
The sectional curvature determines the [[Riemann curvature tensor|curvature tensor]] completely.&lt;br /&gt;
&lt;br /&gt;
==Definition==&lt;br /&gt;
Given a [[Riemannian manifold]] and two [[linearly independent]] [[tangent vectors]] at the same point, &#039;&#039;u&#039;&#039; and &#039;&#039;v&#039;&#039;, we can define&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;K(u,v)={\langle R(u,v)v,u\rangle\over \langle u,u\rangle\langle v,v\rangle-\langle u,v\rangle^2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Here &#039;&#039;R&#039;&#039; is the [[Riemann curvature tensor]].&lt;br /&gt;
&lt;br /&gt;
In particular, if &#039;&#039;u&#039;&#039; and &#039;&#039;v&#039;&#039; are [[orthonormal]], then&lt;br /&gt;
:&amp;lt;math&amp;gt;K(u,v) = \langle R(u,v)v,u\rangle.&amp;lt;/math&amp;gt;&lt;br /&gt;
The sectional curvature in fact depends only on the 2-plane σ&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt; in the tangent space at &#039;&#039;p&#039;&#039; spanned by &#039;&#039;u&#039;&#039; and &#039;&#039;v&#039;&#039;. It is called the &#039;&#039;&#039;sectional curvature of the 2-plane &amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt;&#039;&#039;&#039;, and is denoted &#039;&#039;K&#039;&#039;(&amp;amp;sigma;&amp;lt;sub&amp;gt;&#039;&#039;p&#039;&#039;&amp;lt;/sub&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
==Manifolds with constant sectional curvature==&lt;br /&gt;
&lt;br /&gt;
[[Riemannian manifold]]s with constant sectional curvature are the most simple. These are called [[space form]]s.  By rescaling the metric there are three possible cases&lt;br /&gt;
*negative curvature &amp;amp;minus;1, [[hyperbolic geometry]]&lt;br /&gt;
*zero curvature, [[Euclidean geometry]]&lt;br /&gt;
*positive curvature +1, [[elliptic geometry]]&lt;br /&gt;
The model manifolds for the three geometries are [[hyperbolic space]], [[Euclidean space]] and a unit [[n-sphere|sphere]]. They are the only [[Complete space|complete]], [[simply connected]] Riemannian manifolds of given sectional curvature.  All other connected complete constant curvature manifolds are quotients of those by some group of [[isometry|isometries]].&lt;br /&gt;
&lt;br /&gt;
If for each point in a connected Riemannian manifold (of dimension three or greater) the sectional curvature is independent of the tangent 2-plane, then the sectional curvature is in fact constant on the whole manifold.&lt;br /&gt;
&lt;br /&gt;
==Toponogov&#039;s theorem==&lt;br /&gt;
[[Toponogov&#039;s theorem]] affords a characterization of sectional curvature in terms of how &amp;quot;fat&amp;quot; geodesic triangles appear when compared to their Euclidean counterparts.  The basic intuition is that, if a space is positively curved, then the edge of a triangle opposite some given vertex will tend to bend away from that vertex, whereas if a space is negatively curved, then the opposite edge of the triangle will tend to bend towards the vertex.&lt;br /&gt;
&lt;br /&gt;
More precisely, let &#039;&#039;M&#039;&#039; be a [[complete space|complete]] Riemannian manifold, and let &#039;&#039;xyz&#039;&#039; be a geodesic triangle in &#039;&#039;M&#039;&#039; (a triangle each of whose sides is a length-minimizing geodesic).  Finally, let &#039;&#039;m&#039;&#039; be the midpoint of the geodesic &#039;&#039;xy&#039;&#039;.  If &#039;&#039;M&#039;&#039; has non-negative curvature, then for all sufficiently small triangles&lt;br /&gt;
:&amp;lt;math&amp;gt;d(z,m)^2\ge \tfrac12d(z,x)^2 + \tfrac12d(z,y)^2 - \tfrac14d(x,y)^2&amp;lt;/math&amp;gt;&lt;br /&gt;
where &#039;&#039;d&#039;&#039; is the [[distance function]] on &#039;&#039;M&#039;&#039;.  The case of equality holds precisely when the curvature of &#039;&#039;M&#039;&#039; vanishes, and the right-hand side represents the distance from a vertex to the opposite side of a geodesic triangle in Euclidean space having the same side-lengths as the triangle &#039;&#039;xyz&#039;&#039;.  This makes precise the sense in which triangles are &amp;quot;fatter&amp;quot; in positively curved spaces.  In non-positively curved spaces, the inequality goes the other way:&lt;br /&gt;
:&amp;lt;math&amp;gt;d(z,m)^2\le \tfrac12d(z,x)^2 + \tfrac12d(z,y)^2 - \tfrac14d(x,y)^2.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If tighter bounds on the sectional curvature are known, then this property generalizes to give a [[comparison theorem]] between geodesic triangles in &#039;&#039;M&#039;&#039; and those in a suitable simply connected space form; see [[Toponogov&#039;s theorem]].  Simple consequences of the version stated here are:&lt;br /&gt;
&lt;br /&gt;
*A complete Riemannian manifold has non-negative sectional curvature if and only if the function &amp;lt;math&amp;gt;f_p(x)=\operatorname{dist}^2(p,x)&amp;lt;/math&amp;gt; is 1-[[Glossary of Riemannian and metric geometry|concave]] for all points &#039;&#039;p&#039;&#039;.&lt;br /&gt;
*A complete simply connected Riemannian manifold has non-positive sectional curvature if and only if the function &amp;lt;math&amp;gt;f_p(x)=\operatorname{dist}^2(p,x)&amp;lt;/math&amp;gt; is 1-[[Glossary of Riemannian and metric geometry|convex]].&lt;br /&gt;
&lt;br /&gt;
==Manifolds with non-positive sectional curvature==&lt;br /&gt;
In 1928, [[Élie Cartan]] proved the [[Cartan–Hadamard theorem]]: if &#039;&#039;M&#039;&#039; is a [[Complete space|complete]] manifold with non-positive sectional curvature, then its [[universal cover]] is [[diffeomorphic]] to a [[Euclidean space]]. In particular, it is [[Aspherical space|aspherical]]: the [[homotopy groups]] &amp;lt;math&amp;gt;\pi_i(M)&amp;lt;/math&amp;gt; for &#039;&#039;i&#039;&#039; &amp;amp;ge; 2 are trivial.  Therefore, the topological structure of a complete non-positively curved manifold is determined by its [[fundamental group]].  [[Preissman&#039;s theorem]] restricts the fundamental group of negatively curved compact manifolds.&lt;br /&gt;
&lt;br /&gt;
==Manifolds with positive sectional curvature==&lt;br /&gt;
Little is known about the structure of positively curved manifolds. The [[soul theorem]] ({{harvnb|Cheeger|Gromoll|1972}}; {{harvnb|Gromoll|Meyer|1969}}) implies that a complete non-compact non-negatively curved manifold is diffeomorphic to a normal bundle over a compact non-negatively curved manifold. As for compact positively curved manifolds, there are two classical results:&lt;br /&gt;
&lt;br /&gt;
*It follows from the [[Myers theorem]] that the fundamental group of such manifold is finite.&lt;br /&gt;
&lt;br /&gt;
*It follows from the [[Synge theorem]] that the fundamental group of such manifold in even dimensions is 0, if orientable and &amp;lt;math&amp;gt;\Bbb Z_2&amp;lt;/math&amp;gt; otherwise. In odd dimensions a positively curved manifold is always orientable.&lt;br /&gt;
&lt;br /&gt;
Moreover, there are relatively few examples of compact positively curved manifolds, leaving a lot of conjectures (e.g., the [[Hopf conjecture]] on whether there is a metric of positive sectional curvature on &amp;lt;math&amp;gt;\Bbb S^2\times\Bbb S^2&amp;lt;/math&amp;gt;). The most typical way of constructing new examples is the following corollary from the O&#039;Neill curvature formulas: if &amp;lt;math&amp;gt;(M,g)&amp;lt;/math&amp;gt; is a Riemannian manifold admitting a free isometric action of a Lie group G, and M has positive sectional curvature on all 2-planes orthogonal to the orbits of G, then the manifold &amp;lt;math&amp;gt;M/G&amp;lt;/math&amp;gt; with the quotient metric has positive sectional curvature. This fact allows one to construct the classical positively curved spaces, being spheres and projective spaces, as well as these examples {{harv|Ziller|2007}}:&lt;br /&gt;
&lt;br /&gt;
*The Berger spaces &amp;lt;math&amp;gt;B^7=SO(5)/SO(3)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;B^{13}=SU(5)/Sp(2)\cdot\Bbb S^1&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
*The Wallach spaces (or the homogeneous flag manifolds): &amp;lt;math&amp;gt;W^6=SU(3)/T^2&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;W^{12}=Sp(3)/Sp(1)^3&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;W^{24}=F_4/Spin(8)&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
*The Aloff–Wallach spaces &amp;lt;math&amp;gt;W^7_{p,q}=SU(3)/\operatorname{diag}(z^p,z^q,\overline{z}^{p+q})&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
*The Eschenburg spaces &amp;lt;math&amp;gt;E_{k,l}=\operatorname{diag}(z^{k_1},z^{k_2},z^{k_3})\backslash SU(3)/\operatorname{diag}(z^{l_1},z^{l_2},z^{l_3})^{-1}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*The Bazaikin spaces &amp;lt;math&amp;gt;B^{13}_p=\operatorname{diag}(z_1^{p_1},\dots,z_1^{p_5})\backslash U(5)/\operatorname{diag}(z_2A,1)^{-1}&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;A\in Sp(2)\subset SU(4)&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{Citation | doi=10.2307/1970819 | last1=Cheeger | first1=Jeff | last2=Gromoll | first2=Detlef | title=On the structure of complete manifolds of nonnegative curvature | mr=0309010 | year=1972 | journal=[[Annals of Mathematics|Annals of Mathematics. Second Series]]   | volume=96 | pages=413–443 | issue=3 | publisher=Annals of Mathematics | jstor=1970819}}.&lt;br /&gt;
*{{Citation | doi=10.2307/1970682 | last1=Gromoll | first1=Detlef | last2=Meyer | first2=Wolfgang | title=On complete open manifolds of positive curvature | mr=0247590 | year=1969 | journal=[[Annals of Mathematics|Annals of Mathematics. Second Series]]   | volume=90 | pages=75–90 | issue=1 | publisher=Annals of Mathematics | jstor=1970682}}.&lt;br /&gt;
* {{Citation | last1=Milnor | first1=John Willard | author1-link=John Milnor | title=Morse theory | publisher=[[Princeton University Press]] | series=Based on lecture notes by M. Spivak and R. Wells. Annals of Mathematics Studies, No. 51 | mr=0163331 | year=1963}}.&lt;br /&gt;
* {{Citation | last1=Petersen | first1=Peter | title=Riemannian geometry | publisher=[[Springer-Verlag]] | location=Berlin, New York | edition=2nd | series=Graduate Texts in Mathematics | isbn=978-0-387-29246-5 | mr=2243772 | year=2006 | volume=171}}.&lt;br /&gt;
*{{cite arxiv|first=Wolfgang|last=Ziller|title=Examples of manifolds with non-negative sectional curvature|eprint=math/0701389|year=2007}}.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
&lt;br /&gt;
*[[Riemann curvature tensor]]&lt;br /&gt;
*[[curvature of Riemannian manifolds]]&lt;br /&gt;
*[[curvature]]&lt;br /&gt;
&lt;br /&gt;
{{curvature}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Riemannian geometry]]&lt;br /&gt;
[[Category:Curvature (mathematics)]]&lt;/div&gt;</summary>
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