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In [[differential geometry]] and [[dynamical systems]], a '''closed geodesic''' on a [[Riemannian manifold]] is the projection of a closed orbit of the [[geodesic|geodesic flow]] on the manifold.
 
==Definition==
In a [[Riemannian manifold]] (''M'',''g''), a closed geodesic is a curve <math>\gamma:\mathbb R\rightarrow M</math> that is a [[geodesic]] for the metric ''g'' and is periodic.
 
Closed geodesics can be characterized by means of a variational principle. Denoting by <math>\Lambda M</math> the space of smooth 1-periodic curves on ''M'', closed geodesics of period 1 are precisely the [[critical point (mathematics)|critical points]] of the energy function <math>E:\Lambda M\rightarrow\mathbb R</math>, defined by
 
<math>E(\gamma)=\int_0^1 g_{\gamma(t)}(\dot\gamma(t),\dot\gamma(t))\,\mathrm{d}t.</math>
 
If <math>\gamma</math> is a closed geodesic of period ''p'', the reparametrized curve <math>t\mapsto\gamma(pt)</math> is a closed geodesic of period 1, and therefore it is a critical point of ''E''. If <math>\gamma</math> is a critical point of ''E'', so are the reparametrized curves <math>\gamma^m</math>, for each <math>m\in\mathbb N</math>, defined by <math>\gamma^m(t):=\gamma(mt)</math>. Thus every closed geodesic on ''M'' gives rise to an infinite sequence of critical points of the energy ''E''.
 
==Examples==
On the [[unit sphere]] <math>S^n\subset\mathbb R^{n+1}</math> with the standard round Riemannian metric, every great circle is an example of a closed geodesic. Manifolds all of whose geodesics are closed have been thoroughly investigated in the mathematical literature. On a compact hyperbolic [[surface]], whose fundamental group has no torsion, closed geodesics are in one-to-one correspondence with non-trivial [[conjugacy class]]es of elements in the [[Fuchsian group]] of the surface.
 
==See also==
*[[Selberg trace formula]]
*[[Zoll surface]]
*[[geodesic]]
 
==References==
 
*[[Arthur Besse|Besse, A.]]: "Manifolds all of whose geodesics are closed", ''Ergebisse Grenzgeb. Math.'', no. 93, Springer, Berlin, 1978.
*[[Wilhelm Klingenberg|Klingenberg, W.]]: "Lectures on closed geodesics", Grundlehren der Mathematischen Wissenschaften, Vol. 230. Springer-Verlag, Berlin-New York, 1978. x+227 pp. ISBN 3-540-08393-6
 
[[Category:Differential geometry]]
[[Category:Dynamical systems]]
[[Category:Geodesic (mathematics)]]

Revision as of 23:26, 28 January 2014

In differential geometry and dynamical systems, a closed geodesic on a Riemannian manifold is the projection of a closed orbit of the geodesic flow on the manifold.

Definition

In a Riemannian manifold (M,g), a closed geodesic is a curve that is a geodesic for the metric g and is periodic.

Closed geodesics can be characterized by means of a variational principle. Denoting by the space of smooth 1-periodic curves on M, closed geodesics of period 1 are precisely the critical points of the energy function , defined by

If is a closed geodesic of period p, the reparametrized curve is a closed geodesic of period 1, and therefore it is a critical point of E. If is a critical point of E, so are the reparametrized curves , for each , defined by . Thus every closed geodesic on M gives rise to an infinite sequence of critical points of the energy E.

Examples

On the unit sphere with the standard round Riemannian metric, every great circle is an example of a closed geodesic. Manifolds all of whose geodesics are closed have been thoroughly investigated in the mathematical literature. On a compact hyperbolic surface, whose fundamental group has no torsion, closed geodesics are in one-to-one correspondence with non-trivial conjugacy classes of elements in the Fuchsian group of the surface.

See also

References

  • Besse, A.: "Manifolds all of whose geodesics are closed", Ergebisse Grenzgeb. Math., no. 93, Springer, Berlin, 1978.
  • Klingenberg, W.: "Lectures on closed geodesics", Grundlehren der Mathematischen Wissenschaften, Vol. 230. Springer-Verlag, Berlin-New York, 1978. x+227 pp. ISBN 3-540-08393-6