Carathéodory and Smirnov type theorems for harmonic mappings of the unit disk onto surfaces (Q2860884)
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scientific article; zbMATH DE number 6225486
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Carathéodory and Smirnov type theorems for harmonic mappings of the unit disk onto surfaces |
scientific article; zbMATH DE number 6225486 |
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Carathéodory and Smirnov type theorems for harmonic mappings of the unit disk onto surfaces (English)
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11 November 2013
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Smirnov's theorem
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Carathéodory type theorem
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harmonic mappings
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harmonic surfaces
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isoperimetric inequality
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Riesz-Zygmund inequality.
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0.8963759
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0.88661027
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0.88460016
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0.8822317
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0.87920964
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The authors prove representation theorems which are versions of Smirnov's theorem and Carathéodory type theorems for harmonic homeomorphisms of the unit disk onto Jordan surfaces with rectifiable boundaries. Let \(\Sigma\subseteq{\mathbb R}^n\) be a closed Jordan surface with rectifiable boundary \(\Gamma\), \(\Sigma_o=\Sigma\setminus\Gamma\) and \(f:{\mathbf U}\rightarrow\Sigma_o\) a harmonic homeomorphism of the unit disk \({\mathbf U}\subset\mathbb C\) onto \(\Sigma_o\). Then there exists a function \(\phi:[0,2\pi]\rightarrow\Gamma\), \(\phi(0)=\phi(2\pi)\) with bounded variation and with at most a countable set of points of discontinuity, where it has left and right limits, such that \(f=\text{P}[\phi]\). Here \(\text{P}[\phi]\) is the Poisson integral of \(\phi\). If \(\Gamma\) does not contain any segment, then \(f\) has a continuous extension up to the boundary. If \(\theta_0\in[0,2\pi]\) is a point of discontinuity of \(\phi\), then there exist \(A_0=\lim_{t\uparrow\theta_0}\phi(t)\), \(B_0=\lim_{t\downarrow\theta_0}\phi(t)\) and \(C_{\mathbf U}(f,e^{i\theta_0})=[A_0,B_0]\subseteq\Gamma\). \(C_{\mathbf U}(f,e^{\zeta})\) is the cluster set. The authors establish some classical inequalities for harmonic surfaces. For example, the Riesz-Zygmund inequality for harmonic surfaces. Let \(\Sigma\subseteq{\mathbb R}^n\) be a harmonic Jordan surface which is spanned by a rectifiable curve \(\Gamma\) and parametrized by harmonic coordinates \(\tau\). Then for every \(s\in[0,2\pi]\) NEWLINE\[NEWLINE \int_{-1}^1|\partial_r\tau(re^{is})|\,dt\leqslant\frac12|\Gamma|\,. NEWLINE\]
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