Math 2.0

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 MM be a compact Riemannian manifold without boundary. Let NN be a compact Riemannian manifold whose sectional curvature is nonpositive everywhere.

  1. Let u0,u1 ⁣:M→Nu_0, u_1 \colon M \to N be harmonic maps that are homotopic. Then there is a smooth homotopy utu_t, t∈[0,1]t \in [0, 1], from u0u_0 to u1u_1 such that each utu_t is harmonic and has the same energy as u0u_0. Moreover, for each x∈Mx \in M the curve t↦ut(x)t \mapsto u_t(x) is a geodesic traversed at constant speed, and this speed does not depend on xx.
  2. Suppose that the sectional curvature of NN is negative everywhere. Let u ⁣:M→Nu \colon M \to N be a harmonic map whose image is neither a point nor a closed geodesic. Then uu is the only harmonic map in its homotopy class.

Remarks

Lift to the universal cover of NN, which is a Hadamard manifold, and join u0(x)u_0(x) to u1(x)u_1(x) 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 MM, so it is constant on the compact manifold MM. Following the geodesics gives the homotopy utu_t, and the second variation of the energy shows that every utu_t is again harmonic. With strictly negative curvature the homotopy must be constant, unless all the geodesics t↦ut(x)t \mapsto u_t(x) run along one closed geodesic, which forces the image of uu into that geodesic.

The curvature hypothesis is needed. For M=N=S2M = N = S^2 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 NN, 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.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
  • no evidence level
  1. Energy of a map between Riemannian manifolds concept
  2. Geodesic concept
  3. Harmonic map concept
  4. Harmonic map heat flow concept
  5. Homotopy concept
  6. Riemannian manifold concept
  7. Sectional curvature concept
  8. Eells–Sampson theorem statement
  9. Hartman's uniqueness theorem for harmonic maps statement

Further reading

  1. Web https://en.wikipedia.org/wiki/Harmonic_map
About this page
Tag3VMJGQCD7S
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Kindstatement, theorem
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MSC58E20, 53C43
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AboutHarmonic map
UsesHarmonic map, Riemannian manifold, Sectional curvature, Homotopy, Geodesic, Energy of a map between Riemannian manifolds, Eells–Sampson theorem

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