1996
DOI: 10.4310/jdg/1214459224
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Bubble tree convergence for harmonic maps

Abstract: Let Σ be a compact Riemann surface. Any sequence f n : Σ -> M of harmonic maps with bounded energy has a "bubble tree limit" consisting of a harmonic map /o : Σ -> M and a tree of bubblesWe give a precise construction of this bubble tree and show that the limit preserves energy and homotopy class, and that the images of the f n converge pointwise. We then give explicit counterexamples showing that bubble tree convergence fails (i) for harmonic maps f n when the conformal structure of Σ varies with n, and (ii) … Show more

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Cited by 155 publications
(175 citation statements)
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“…In the case s ¼ 2 we mention in particular the papers [13], [10] and [15]. Parker's paper [13] was the first to present a ''bubble tree analysis'', in this case for an equibounded sequence of harmonic maps from a 2-dimensional manifold; his results basically show that such a sequence can be associated to a limiting configuation, a ''bubble tree'', consisting of a harmonic map f 0 : M ! N and a tree of bubbles f k : S 2 !…”
Section: Introductionmentioning
confidence: 99%
“…In the case s ¼ 2 we mention in particular the papers [13], [10] and [15]. Parker's paper [13] was the first to present a ''bubble tree analysis'', in this case for an equibounded sequence of harmonic maps from a 2-dimensional manifold; his results basically show that such a sequence can be associated to a limiting configuation, a ''bubble tree'', consisting of a harmonic map f 0 : M ! N and a tree of bubbles f k : S 2 !…”
Section: Introductionmentioning
confidence: 99%
“…When the domain is two-dimensional, particularly interesting features arise. The conformal invariance of the energy functional leads to non-compactness of the set of harmonic maps in dimension two, and the blow-up behavior has been studied extensively in [5,13,20,23,24,27] for the interior case and [10,15,16] for the boundary case. Roughly speaking, the energy identities for harmonic maps tell us that, during the weak convergence of a sequence of harmonic maps, the loss of energy is concentrated at finitely many points and can be quantized by a sum of energies of harmonic spheres and harmonic disks.…”
Section: Introductionmentioning
confidence: 99%
“…This means that the loss of energy under the limiting process can be recovered by the energy of a finite number of bubbles. Readers can refer to the pioneering work on the energy identity by Jost [18], Parker [22] regarding the harmonic maps from surfaces and by Ding-Tian [6] for the harmonic map flow. For n-harmonic maps with n ≥ 3, the isolated singularities are removable due to Duzaar-Fuchs [7] and the energy identity was provided by Wang-Wei [27] for a sequence of approximate n-harmonic maps.…”
Section: Introductionmentioning
confidence: 99%