In mathematics, Carathéodory's theorem is a theorem in complex analysis, named after Constantin Carathéodory, which extends the Riemann mapping theorem. The theorem, first proved in 1913, states that the conformal mapping sending the unit disk to the region in the complex plane bounded by a Jordan curve extends continuously to a homeomorphism from the unit circle onto the Jordan curve. The result is one of Carathéodory's results on prime ends and the boundary behaviour of univalent holomorphic functions.
Proofs of Carathéodory's theorem
The first proof of Carathéodory's theorem presented here is a summary of the short self-contained account in Garnett & Marshall (2005, pp. 14–15); there are related proofs in Pommerenke (1992) and Krantz (2006).
Carathéodory's theorem. If f maps the open unit disk D conformally onto a bounded domain U in C, then f has a continuous one-to-one extension to the closed unit disk if and only if ∂U is a Jordan curve.
Clearly if f admits an extension to a homeomorphism, then ∂U must be a Jordan curve.
Conversely if ∂U is a Jordan curve, the first step is to prove f extends continuously to the closure of D. In fact this will hold if and only if f is uniformly continuous on D: for this is true if it has a continuous extension to the closure of D; and, if f is uniformly continuous, it is easy to check f has limits on the unit circle and the same inequalities for uniform continuity hold on the closure of D.
Suppose that f is not uniformly continuous. In this case there must be an ε > 0 and a point ζ on the unit circle and sequences zn, wn tending to ζ with |f(zn) − f(wn)| ≥ 2ε. This is shown below to lead to a contradiction, so that f must be uniformly continuous and hence has a continuous extension to the closure of D.
For 0 < r < 1, let γr be the curve given by the arc of the circle | z − ζ | = r lying within D. Then f ∘ γr is a Jordan curve. Its length can be estimated using the Cauchy–Schwarz inequality:
\( {\displaystyle \displaystyle {\ell (f\circ \gamma _{r})=\int _{\gamma _{r}}|f^{\prime }(z)|\,|dz|\leq \left(\int _{\gamma _{r}}\,|dz|\right)^{1/2}\cdot \left(\int _{\gamma _{r}}|f^{\prime }(z)|^{2}\,|dz|\right)^{1/2}\leq (2\pi r)^{1/2}\cdot \left(\int _{\{\theta :|\zeta +re^{i\theta }|<1\}}|f^{\prime }(\zeta +re^{i\theta })|^{2}\,r\,d\theta \right)^{1/2}.}} \)
Hence there is a "length-area estimate":
\( {\displaystyle \displaystyle {\int _{0}^{1}\ell (f\circ \gamma _{r})^{2}\,{dr \over r}\leq 2\pi \int _{|z|<1}|f^{\prime }(z)|^{2}\,dx\,dy=2\pi \cdot {\rm {Area}}\,f(D)<\infty .}} \)
The finiteness of the integral on the left hand side implies that there is a sequence rn decreasing to 0 with \( {\displaystyle \ell (f\circ \gamma _{r_{n}})} \) tending to 0. But the length of a curve g(t) for t in (a, b) is given by
\( {\displaystyle \displaystyle {\ell (g)=\sup _{a<t_{1}<t_{2}<\cdots <t_{k}<b}\sum _{i=1}^{k-1}|g(t_{i+1})-g(t_{i})|.}}\) \)
The finiteness of \( {\displaystyle \ell (f\circ \gamma _{r_{n}})} \) therefore implies that the curve has limiting points an, bn at its two ends with \( {\displaystyle \ell (f\circ \gamma _{r_{n}})} \), so this difference tends to 0. These two limit points must lie on ∂U, because f is a homeomorphism between D and U and thus a sequence converging in U has to be the image under f of a sequence converging in D. Since ∂U is a homeomorphic image of the circle ∂D, the distance between the two corresponding parameters ξn and ηn in ∂U must tend to 0. So eventually the smallest circular arc in ∂D joining ξn and ηn is defined and, by uniform continuity, the diameter of its image τn tends to 0. Together τn and f ∘ γrn form a simple Jordan curve. Its interior Un is contained in U by the Jordan curve theorem for ∂U and ∂Un: to see this, notice that U is the interior of ∂U, as it is bounded, connected and it is both open and closed in the complement of ∂U; so the exterior region of ∂U is unbounded, connected and does not intersect ∂Un, hence its closure is contained in the closure of the exterior of ∂Un; taking complements, we get the desired inclusion. The diameter of ∂Un tends to 0 because the diameters of τn and f ∘ γrn tend to 0. Hence the diameter and the area of Un tend to 0.
Now if Vn denotes the intersection of D with the disk |z − ζ| < rn, then f(Vn) = Un. Indeed, the arc γrn divides D into Vn and a complementary region; Un is a connected component of U \ f ∘ γrn, as it is connected and is both open and closed in this set, so under the conformal homeomorphism f the curve f ∘ γrn divides U into Un and a complementary region Un′, one of which equals f(Vn). Since the areas of f(Vn) and Un tend to 0, while the sum of the areas of Un and Un′ is fixed, it follows that f(Vn) = Un.
So the diameter of f(Vn) tends to 0. On the other hand, passing to subsequences of (zn) and (wn) if necessary, it may be assumed that zn and wn both lie in Vn. But this gives a contradiction since |f(zn) − f(wn)| ≥ ε. So f must be uniformly continuous on U.
Thus f extends continuously to the closure of D. Since f(D) = U, by compactness f carries the closure of D onto the closure of U and hence ∂D onto ∂U. If f is not one-one, there are points u, v on ∂D with u ≠ v and f(u) = f(v). Let X and Y be the radial lines from 0 to u and v. Then f(X ∪ Y) is a Jordan curve. Arguing as before, its interior V is contained in U and is a connected component of U \ f(X ∪ Y). On the other hand, D \ (X ∪ Y) is the disjoint union of two open sectors W1 and W2. Hence, for one of them, W1 say, f(W1) = V. Let Z be the portion of ∂W1 on the unit circle, so that Z is a closed arc and f(Z) is a subset of both ∂U and the closure of V. But their intersection is a single point and hence f is constant on Z. By the Schwarz reflection principle, f can be analytically continued by conformal reflection across the circular arc. Since non-constant holomorphic functions have isolated zeros, this forces f to be constant, a contradiction. So f is one-one and hence a homeomorphism on the closure of D.[1][2]
Two different proofs of Carathéodory's theorem are described in Carathéodory (1954) and Carathéodory (1998). The first proof follows Carathéodory's original method of proof from 1913 using properties of Lebesgue measure on the circle: the continuous extension of the inverse function g of f to ∂U is justified by Fatou's theorem on the boundary behaviour of bounded harmonic functions on the unit disk. The second proof is based on the method of Lindelöf (1914), where a sharpening of the maximum modulus inequality was established for bounded holomorphic functions h defined on a bounded domain V: if a lies in V, then
|h(a)| ≤ mt ⋅ M1 − t,
where 0 ≤ t ≤ 1, M is maximum modulus of h for sequential limits on ∂U and m is the maximum modulus of h for sequential limits on ∂U lying in a sector centred on a subtending an angle 2πt at a.[3]
Continuous extension and the Carathéodory-Torhorst theorem
An extension of the theorem states that a conformal isomorphism
\( {\displaystyle g\colon \mathbb {D} \to U}, \)
where U {\displaystyle U} U is a simply connected subset of the Riemann sphere, extends continuously to the unit circle if and only if the boundary of U {\displaystyle U} U is locally connected.
This result is often also attributed to Carathéodory, but was first stated and proved by Marie Torhorst in her 1918 thesis,[4] under the supervision of Hans Hahn, using Carathéodory's theory of prime ends. More precisely, Torhorst proved that local connectivity is equivalent to the domain having only prime ends of the first kind. By the theory of prime ends, the latter property, in turn, is equivalent to g {\displaystyle g} g having a continuous extension.
Notes
Krantz 2006, pp. 116–117
Garnett & Marshall 2005, p. 15
Ahlfors 2010, pp. 37–40
Torhorst, Marie (1921), "Über den Rand der einfach zusammenhängenden ebenen Gebiete", Mathematische Zeitschrift, 9 (1–2): 44–65, doi:10.1007/BF01378335, S2CID 120418797
References
Carathéodory, C. (1913a), "Zur Ränderzuordnung bei konformer Abbildung", Göttingen Nachrichten: 509–518
Carathéodory, C. (1913b), "Über die gegenseitige Beziehung der Ränder bei der konformen Abbildung des Inneren einer Jordanschen Kurve auf einen Kreis", Mathematische Annalen, Springer Berlin / Heidelberg, 73 (2): 305–320, doi:10.1007/BF01456720, ISSN 0025-5831, JFM 44.0757.01, S2CID 117117051
Carathéodory, C. (1954), Theory of functions of a complex variable, Vol. 2, translated by F. Steinhardt, Chelsea
Carathéodory, C. (1998), Conformal representation (reprint of the 1952 second edition), Dover, ISBN 0-486-40028-X
Lindelöf, E. (1914), "Sur la représentation conforme", Comptes Rendus de l'Académie des Sciences, Paris, 158: 245–247
Lindelöf, E. (1916), "Sur la représentation conforme d'une aire simplement connexe sur l'aire d'un cercle", 4th International Congress of Scandinavian Mathematicians, pp. 59–90
Ahlfors, Lars V. (2010), Conformal invariants: topics in geometric function theory, AMS Chelsea Publishing, ISBN 978-0-8218-5270-5
Garnett, John B.; Marshall, Donald E. (2005), Harmonic measure, New Mathematical Monographs, 2, Cambridge University Press, ISBN 0-521-47018-8
Goluzin, G. M. (1969), Geometric theory of functions of a complex variable, Translations of Mathematical Monographs, 26, American Mathematical Society
Krantz, Steven G. (2006), Geometric function theory: explorations in complex analysis, Birkhäuser, ISBN 0-8176-4339-7
Markushevich, A. I. (1977), Theory of functions of a complex variable. Vol. III, Chelsea Publishing Co., ISBN 0-8284-0296-5, MR 0444912
Pommerenke, C. (1975), Univalent functions, with a chapter on quadratic differentials by Gerd Jensen, Studia Mathematica/Mathematische Lehrbücher, 15, Vandenhoeck & Ruprecht
Pommerenke, C. (1992), Boundary behaviour of conformal maps, Grundlehren der Mathematischen Wissenschaften, 299, Springer, ISBN 3-540-54751-7
Shields, Allen (1988), "Carathéodory and conformal mapping", The Mathematical Intelligencer, 10 (1): 18–22, doi:10.1007/BF03023846, ISSN 0343-6993, MR 0918659, S2CID 189887440
Whyburn, Gordon T. (1942), Analytic Topology, American Mathematical Society Colloquium Publications, 28, American Mathematical Society
Undergraduate Texts in Mathematics
Graduate Studies in Mathematics
Hellenica World - Scientific Library
Retrieved from "http://en.wikipedia.org/"
All text is available under the terms of the GNU Free Documentation License
