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Titlebook: Constant Mean Curvature Surfaces, Harmonic Maps and Integrable Systems; Frédéric Hélein Book 2001 Springer Basel AG 2001 Finite.Loop group

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Overview: 978-3-7643-6576-9978-3-0348-8330-6
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Three Lectures on QCD Phase Transitionse this property of . is invariant by conformal changes of variables, one might be interested in the behaviour of . by such a transformation. So let’s choose a conformal mapwhere Ω. is the domain of a map .:and let’s check how the corresponding function . transforms. We writefor the coordinates of Ω. and Ω., respectively. Set Compute
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Heavy Flavors and Exotic HadronsWood in 1982 [34], F. Burstall and J. H. Rawnsley in 1986 [23], and K. Uhlenbeck in 1989 [82]. We are going to consider harmonic maps .: . → . ⊂ ℝ., i. e. maps satisfyingwhich is equivalent to Δ. ∥ .. In contrast to Chapter 4, where we considered the Hopf differentialwe will also use derivatives of
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https://doi.org/10.1007/978-3-030-95534-2ow that for CMC tori, all such harmonic maps are of finite type, a result of U. Pinkall and I. Sterling. This result can be generalized to harmonic maps from torus into Lie groups [21] or more generally into symmetric spaces [21], [22].
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https://doi.org/10.1007/978-3-030-95534-2resch simplified this construction. He remarked that Wente tori should possess planar curvature lines and thus studied all CMC surfaces with planar curvature lines. It leads to an overdetermined system of equations which can be solved by quadratures using elliptic integrals. And U. Abresch showed th
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Constant mean curvature tori are of finite type,ow that for CMC tori, all such harmonic maps are of finite type, a result of U. Pinkall and I. Sterling. This result can be generalized to harmonic maps from torus into Lie groups [21] or more generally into symmetric spaces [21], [22].
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https://doi.org/10.1007/978-3-0348-8330-6Finite; Loop group; Meromorphic function; Microsoft Access; algebra; constant; curvature; differential geom
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