Global analysis, analysis on manifolds Harmonic maps and gauge-theoretic variational problems Theorem
Hartman's uniqueness theorem for harmonic maps
Builds on Harmonic mapRiemannian manifoldSectional curvatureHomotopyGeodesicEnergy of a map between Riemannian manifoldsEells–Sampson theorem
Statement
Let be a compact Riemannian manifold without boundary. Let be a compact Riemannian manifold whose sectional curvature is nonpositive everywhere.
- Let be harmonic maps that are homotopic. Then there is a smooth homotopy , , from to such that each is harmonic and has the same energy as . Moreover, for each the curve is a geodesic traversed at constant speed, and this speed does not depend on .
- Suppose that the sectional curvature of is negative everywhere. Let be a harmonic map whose image is neither a point nor a closed geodesic. Then is the only harmonic map in its homotopy class.
Remarks
Lift to the universal cover of , which is a Hadamard manifold, and join to by the unique geodesic in the right homotopy class. In nonpositive curvature the squared distance between the two lifted maps is a subharmonic function on , so it is constant on the compact manifold . Following the geodesics gives the homotopy , and the second variation of the energy shows that every is again harmonic. With strictly negative curvature the homotopy must be constant, unless all the geodesics run along one closed geodesic, which forces the image of into that geodesic.
The curvature hypothesis is needed. For with the round metric, every rotation is a harmonic map homotopic to the identity. So harmonic maps in a homotopy class are far from unique. Uniqueness also fails in the flat case: on a flat torus , composing a harmonic map with a translation gives a family of homotopic harmonic maps, as part 1 allows.
Going deeper
For a student
The theorem complements the Eells–Sampson theorem, which gives existence of a harmonic map in each homotopy class under the same curvature hypothesis. Together they say that, for targets of negative curvature, a homotopy class of maps usually has a canonical harmonic representative. This is used in rigidity theory, for example for maps between locally symmetric spaces and in the study of Teichmüller space.
Reading path
To understand this page from the ground up, read these 9 pages in order. The foundations come first.
Show the path as a graph
- no evidence level
- Energy of a map between Riemannian manifolds concept
- Geodesic concept
- Harmonic map concept
- Harmonic map heat flow concept
- Homotopy concept
- Riemannian manifold concept
- Sectional curvature concept
- Eells–Sampson theorem statement
- Hartman's uniqueness theorem for harmonic maps statement
Further reading
About this page
| Tag | 3VMJGQCD7S |
|---|---|
| URI | m2://3VMJGQCD7S |
| Kind | statement, theorem |
| Writing | W0 stub |
| MSC | 58E20, 53C43 |
| Status | This copy of the site has no build data. Run m2 status 3VMJGQCD7S. |
| About | Harmonic map |
| Uses | Harmonic map, Riemannian manifold, Sectional curvature, Homotopy, Geodesic, Energy of a map between Riemannian manifolds, Eells–Sampson theorem |
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