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Lars Ahlfors

Lars Valerian Ahlfors

A course on the Finnish analyst who won one of the first two Fields Medals, turned value distribution theory into geometry, and with Lipman Bers built the modern theory of quasiconformal maps, Teichmüller spaces and Kleinian groups.

Born 18 April 1907, Helsinki Died 11 October 1996, Pittsfield, Massachusetts Fields Medal Oslo, 1936 Level advanced undergraduate → graduate
Images of four disjoint circles under the group generated by reflections in them. The circles accumulate on a Cantor-like limit set. Ahlfors conjectured that the limit set of any finitely generated Kleinian group has either zero area or is the whole sphere.
Lesson 00

How to use this course

Lars Ahlfors worked in complex analysis for nearly seventy years. His career falls into two periods. Before the Second World War he solved Denjoy’s conjecture, recast Rolf Nevanlinna’s value distribution theory as the geometry of covering surfaces, and generalized Schwarz’s lemma to curved metrics. After the war, at Harvard, he made quasiconformal mappings a central subject, gave the first complete proofs of Oswald Teichmüller’s theorems, and opened the modern study of Kleinian groups. His textbook Complex Analysis has taught the subject to generations of students.

Prerequisites for Part II
  • A first course in complex analysis: Cauchy’s theorem, conformal mapping, the Schwarz lemma, harmonic functions.
  • Basic differential geometry of surfaces: Gaussian curvature, the Gauss–Bonnet formula.
  • For Lessons 08–10, some hyperbolic geometry and the definition of a Riemann surface.

Each technical lesson opens with a paragraph for the general reader, then gives precise statements, proof sketches and exercises with folded solutions. The lessons follow his work in order: entire functions (1929), covering surfaces (1935), curvature (1938), conformal invariants (1947–1950), quasiconformal maps (1953–1963) and Kleinian groups (1964 onward).

Reference

Timeline

1907Born 18 April in Helsingfors (Helsinki), Grand Duchy of Finland. His mother dies at his birth; he spends his first years with aunts in the Åland Islands.
1924Enters the University of Helsinki; studies with Ernst Lindelöf and Rolf Nevanlinna.
1928Master’s examinations. Autumn: follows Nevanlinna to Zürich, where Nevanlinna replaces Hermann Weyl for a year.
1929Proves Denjoy’s conjecture on asymptotic values of entire functions.
1930Doctorate at Helsinki, after a year as lecturer at Åbo Akademi in Turku.
1930–32Travels in Europe; Rockefeller fellowship in Paris.
1933Adjunct professor at Helsinki. Marries Erna Lehnert.
1935Zur Theorie der Überlagerungsflächen, Acta Mathematica. Three-year appointment at Harvard.
1936One of the first two Fields Medals, with Jesse Douglas, at the ICM in Oslo.
1938Professor at Helsinki. An extension of Schwarz’s lemma.
1939–44Wartime in Helsinki; family evacuated to Sweden.
1945Professor in Zürich.
1946Returns to Harvard for the rest of his career.
1947Bounded analytic functions: analytic capacity.
1950With Arne Beurling, Conformal invariants and function-theoretic null-sets.
1953Complex Analysis. On quasiconformal mappings (1953–54): Teichmüller’s theorem proved.
1960With Lipman Bers, Riemann’s mapping theorem for variable metrics. Riemann Surfaces with Leo Sario.
1963Quasiconformal reflections.
1964Finiteness theorem for Kleinian groups. William Caspar Graustein Professor.
1968Wihuri International Prize.
1977Retires from Harvard.
1981Wolf Prize, shared with Oscar Zariski.
1982Steele Prize of the American Mathematical Society; Collected Papers.
1986Honorary president of the ICM in Berkeley.
1996Dies 11 October in Pittsfield, Massachusetts, aged 89.
Part I · Formation
Lesson 01

Helsingfors, 1907–1928

Lars Valerian Ahlfors was born on 18 April 1907 in Helsingfors, the Swedish name of Helsinki, then capital of a grand duchy of the Russian Empire. His mother died giving birth to him. He spent his first years with two aunts in the Åland Islands before returning to his father, Axel Ahlfors, a professor of mechanical engineering. The family spoke Swedish, and Lars attended a private Swedish-language school. He later became nearly fluent in Finnish, German and English.

Finland declared independence in 1917 and fell into civil war in 1918. Food was short, and his father was briefly imprisoned by the Red Guard. The boy taught himself mathematics from his sister’s homework and from his father’s engineering books, which included calculus. His school did not teach it.

He entered the University of Helsinki in 1924. Finland had a remarkable school of complex function theory founded by Ernst Lindelöf, and Ahlfors studied with Lindelöf and with Rolf Nevanlinna, who had recently created the theory of value distribution of meromorphic functions. Ahlfors completed his master’s examinations in the spring of 1928.

Lesson 02

Zürich and Denjoy’s conjecture, 1928–1930

In the autumn of 1928 Nevanlinna was invited to the ETH in Zürich to replace Hermann Weyl, who was away for a year. Ahlfors went with him. He later described the move as going from the periphery to the centre of Europe. In Zürich he attended Nevanlinna’s lectures and decided to become a research mathematician.

Nevanlinna lectured on a problem posed by Arnaud Denjoy in 1907: an entire function of finite order \(\rho\) should have at most \(2\rho\) distinct finite asymptotic values. Torsten Carleman had proved a weaker bound. Ahlfors found a proof of the full conjecture using conformal mapping of strip-like domains, a method whose key estimate is now called the Ahlfors distortion theorem (Lesson 04). He published it in 1929, at 22, and was immediately known to every function theorist in Europe.

He spent 1929–30 as a lecturer at Åbo Akademi, the Swedish-language university in Turku, and defended his doctoral thesis at Helsinki in the spring of 1930, with Lindelöf and Nevanlinna as his teachers.

Lesson 03

Paris, Turku, Harvard, Oslo, 1930–1938

From 1930 to 1932 Ahlfors travelled on the Continent, with a long stay in Paris on a Rockefeller Foundation fellowship. In 1933 he became an adjunct professor at the University of Helsinki and married Erna Lehnert, an Austrian. He later called the marriage the happiest event of his life.

In 1935 he published Zur Theorie der Überlagerungsflächen in Acta Mathematica. It rebuilt Nevanlinna theory as a theory of covering surfaces of the sphere, using only metric and topological arguments. The paper also used maps with bounded distortion, under the name quasiconformal mappings, which Herbert Grötzsch had introduced in 1928.

That year, on the recommendation of Constantin Carathéodory, Harvard offered him a three-year appointment. At the International Congress in Oslo in July 1936, the first two Fields Medals were awarded, to Ahlfors and to Jesse Douglas of MIT. Ahlfors learned of the prize only hours before the ceremony. The committee cited above all his work on covering surfaces and called him one of the most brilliant representatives of Lindelöf’s Finnish school.

In 1938 he accepted a chair at Helsinki, from loyalty to his teachers and his country. In the same year he published a short paper extending Schwarz’s lemma to metrics of negative curvature. It became one of the most cited results in geometric function theory (Lesson 06).

Part II · The mathematics
Lesson 04

Asymptotic values and the distortion theorem

For the general reader. An entire function, such as \(e^z\), is defined on the whole complex plane. Along some paths to infinity it may approach a fixed value. Denjoy guessed that slowly growing functions have few such limiting values. Ahlfors proved it by measuring how much a narrow, winding channel must be stretched when it is straightened out into a strip.

Goals
  • State the Denjoy–Carleman–Ahlfors theorem.
  • State the distortion theorem and see how it bounds growth.
  • Check sharpness with explicit functions.

Let \(f\) be entire with maximum modulus \(M(r)=\max_{|z|=r}|f(z)|\). Its order is \(\rho=\limsup_{r\to\infty}\frac{\log\log M(r)}{\log r}\). A value \(a\in\mathbb C\) is an asymptotic value if \(f(\gamma(t))\to a\) along some path \(\gamma(t)\to\infty\).

Theorem (Denjoy–Carleman–Ahlfors, 1929)

An entire function of order \(\rho<\infty\) has at most \(2\rho\) distinct finite asymptotic values.

The distortion theorem

Let \(\Omega\) be a domain lying in a strip around the positive real axis, and suppose each vertical line \(\operatorname{Re}z=x\) meets \(\Omega\) in a cross-cut of length \(\theta(x)\). Let \(F\) map \(\Omega\) conformally onto the strip \(\{0<\operatorname{Im}w<1\}\), with the two ends corresponding.

Ahlfors distortion theorem (1930)

If \(\int_{x_1}^{x_2}\frac{dx}{\theta(x)}>2\), then every point of the cross-cut at \(x_2\) lies further along the strip than every point of the cross-cut at \(x_1\), by at least

\[ \int_{x_1}^{x_2}\frac{dx}{\theta(x)}-4 . \]

For a straight strip of width \(\theta\), the map is \(w=z/\theta\) and the advance is exactly \(\int dx/\theta\). The theorem says a winding channel is never conformally shorter than its width profile suggests, up to a fixed error. Its modern proof uses extremal length (Lesson 07).

Proof idea for Denjoy

Suppose \(f\) has \(n\) distinct finite asymptotic values. Between the asymptotic paths lie \(n\) disjoint unbounded domains \(D_k\) on which \(\log|f|\) is large and tends to infinity. In logarithmic coordinates \(\zeta=\log z\), each \(D_k\) becomes a channel whose cross-cut at \(\operatorname{Re}\zeta=\log r\) has length \(\theta_k(r)\), with \(\sum_k\theta_k(r)\le2\pi\). Harmonic-measure estimates plus the distortion theorem give \(\log\log M(r)\ge\pi\int^{r}\frac{dt}{t\,\theta_k(t)}-C\) for each \(k\). By Cauchy–Schwarz, \(\sum_k1/\theta_k\ge n^2/\sum_k\theta_k\ge n^2/(2\pi)\), so for some \(k\), along a sequence of radii, the integral is at least \(\frac{n}{2\pi}\log r\) up to constants. Hence \(\log\log M(r)\ge\frac n2\log r-C'\), and \(\rho\ge n/2\).

Exercise 4.1Show that the sine integral \(\operatorname{Si}(z)=\int_0^z\frac{\sin t}{t}\,dt\) is entire of order 1 and has the two finite asymptotic values \(\pm\pi/2\). So the bound \(2\rho\) is attained.

Show solution
\(\sin t/t\) is entire, so \(\operatorname{Si}\) is entire; its Taylor coefficients behave like those of \(\sin\), and \(|\operatorname{Si}(z)|\le C e^{|z|}\), so the order is 1 (it is not of order below 1, because \(\operatorname{Si}'\) has order 1). Along the positive real axis \(\operatorname{Si}(x)\to\int_0^\infty\frac{\sin t}{t}dt=\pi/2\). The function is odd, so it tends to \(-\pi/2\) along the negative axis. Two values, and \(2\rho=2\).

Exercise 4.2Generalize: for an integer \(q\ge1\), \(f(z)=\int_0^z\frac{\sin(t^q)}{t^q}\,dt\) has order \(q\). Find \(2q\) distinct finite asymptotic values.

Show solution
Let \(\omega^{2q}=1\), so \(\omega^q=\pm1\). On the ray \(t=\omega s\), \(s>0\): \(t^q=\pm s^q\) and \(\sin(\pm s^q)/(\pm s^q)=\sin(s^q)/s^q\). Hence \(f(\omega s)=\omega\int_0^s\frac{\sin(u^q)}{u^q}du\to\omega C\), where \(C=\int_0^\infty\frac{\sin(u^q)}{u^q}du\) converges and is positive. The \(2q\) roots \(\omega\) give \(2q\) distinct values \(\omega C\). The order is that of \(\sin(z^q)\), namely \(q\).

Exercise 4.3What are the asymptotic values of \(e^z\)? Is the theorem’s bound attained?

Show solution
Along the negative real axis \(e^z\to0\), and along any path with \(\operatorname{Re}z\to-\infty\) the limit is 0. Along paths with bounded real part \(e^z\) has no limit, and along \(\operatorname{Re}z\to+\infty\) it tends to \(\infty\), which is not finite. So there is one finite asymptotic value, while \(2\rho=2\). The bound is not attained.
Lesson 05

Covering surfaces and the five islands

For the general reader. Picard’s theorem says a non-constant entire function takes every complex value with at most one exception. Nevanlinna turned this into precise counting formulas. Ahlfors found that the heart of Nevanlinna’s theory is a fact about how a surface can be spread over a sphere, and that it is close to the Euler characteristic of topology. This is the work that won the Fields Medal.

Goals
  • Define the mean sheet number and the relative boundary length.
  • State Ahlfors’ second main theorem for covering surfaces.
  • Deduce the five islands theorem.

Let \(f\) be meromorphic on a domain containing the closed disc \(|z|\le r\), regarded as a map to the Riemann sphere \(\hat{\mathbb C}\) with its spherical metric of total area \(4\pi\). Define

\[ S(r)=\frac{1}{4\pi}\iint_{|z|<r}\frac{4|f'(z)|^2}{(1+|f(z)|^2)^2}\,dx\,dy,\qquad L(r)=\int_{|z|=r}\frac{2|f'(z)|}{1+|f(z)|^2}\,|dz| . \]

\(S(r)\) is the spherical area of the image counted with multiplicity, divided by the area of the sphere: the mean sheet number. \(L(r)\) is the spherical length of the image of the boundary circle. Let \(D_1,\dots,D_q\) be Jordan domains on the sphere with pairwise disjoint closures. An island over \(D_\nu\) is a component of \(f^{-1}(D_\nu)\) whose closure lies in \(|z|<r\); it is simple if \(f\) maps it one-to-one onto \(D_\nu\).

Ahlfors’ second main theorem (1935)

There is a constant \(h\) depending only on \(D_1,\dots,D_q\) such that

\[ (q-2)\,S(r)\ \le\ \sum_{\nu=1}^{q} n(r,D_\nu)+h\,L(r), \]

where \(n(r,D_\nu)\) is the number of simply connected islands over \(D_\nu\) in \(|z|<r\).

The number \(q-2\) is minus the Euler characteristic of the sphere with \(q\) holes, and the proof is a careful comparison of Euler characteristics, with \(hL\) bounding the error from pieces that touch the boundary. Ahlfors also proved the length–area principle: if \(f\) is meromorphic in the plane and non-constant, then \(L(r)=o(S(r))\) as \(r\to\infty\) outside a set of \(r\) of finite logarithmic measure. In this sense the boundary is negligible.

Five islands theorem (Ahlfors, 1935)

Let \(f\) be a non-constant meromorphic function in \(\mathbb C\), and \(D_1,\dots,D_5\) Jordan domains on the sphere with disjoint closures. Then for some \(\nu\), \(f\) has a simple island over \(D_\nu\). For entire functions, three domains in \(\mathbb C\) suffice.

Proof sketch from the main theorem. Suppose no island over any \(D_\nu\) is simple, so every simply connected island covers \(D_\nu\) at least twice. The islands over \(D_\nu\) cover it at most \(S(r)+O(L(r))\) times in total, so \(n(r,D_\nu)\le\tfrac12 S(r)+O(L(r))\). Then \(3S\le\tfrac52S+O(L)\), that is, \(\tfrac12S(r)=O(L(r))\), contradicting \(L=o(S)\).

Exercise 5.1For \(f(z)=z^n\), compute \(S(r)\) and \(L(r)\) and check that \(L(r)/S(r)\to0\).

Show solution
The image of \(|z|<r\) covers the disc \(|w|<r^n\) exactly \(n\) times. Its spherical area is \(4\pi r^{2n}/(1+r^{2n})\), so \(S(r)=n\,r^{2n}/(1+r^{2n})\to n\). The boundary goes \(n\) times round the circle \(|w|=r^n\), whose spherical length is \(2\pi\cdot2r^n/(1+r^{2n})\), so \(L(r)=4\pi n r^n/(1+r^{2n})\to0\). Hence \(L/S\to0\).

Exercise 5.2Show that “five” cannot be replaced by “four” for meromorphic functions. Hint: use a Weierstrass \(\wp\)-function, which satisfies \(\wp'^2=4(\wp-e_1)(\wp-e_2)(\wp-e_3)\).

Show solution
The critical values of \(\wp\) are \(e_1,e_2,e_3\) and \(\infty\): every preimage of these points is a critical point (\(\wp'=0\), or a double pole). Take small discs \(D_\nu\) around these four values. Any island over \(D_\nu\) contains a preimage of the centre, which is a critical point, so \(f\) is not injective there. No island is simple.
Lesson 06

Ahlfors’ lemma and Bloch’s constant

For the general reader. Schwarz’s lemma says that a holomorphic map of the unit disc into itself cannot increase hyperbolic distances. In 1938 Ahlfors saw that this is really a statement about curvature: any metric on the disc that is at least as negatively curved as the hyperbolic metric must be smaller than it. This idea later grew into Kobayashi hyperbolicity and much of complex geometry.

Goals
  • Define the curvature of a conformal metric.
  • Prove Ahlfors’ lemma by the maximum principle.
  • Recover Schwarz–Pick and see the application to Bloch’s theorem.

A conformal metric \(\lambda(z)|dz|\) with \(\lambda>0\) of class \(C^2\) has Gaussian curvature

\[ K_\lambda=-\frac{\Delta\log\lambda}{\lambda^2}. \]

The Poincaré metric on the unit disc \(\mathbb D\) is \(\lambda_{\mathbb D}=\frac{2}{1-|z|^2}\), with \(K\equiv-1\).

Ahlfors’ lemma (1938)

Let \(\lambda(z)|dz|\) be a conformal metric on \(\mathbb D\) (allowed to vanish at isolated points) with \(K_\lambda\le-1\) wherever \(\lambda>0\). Then \(\lambda(z)\le\frac{2}{1-|z|^2}\) on \(\mathbb D\).

Proof

Fix \(0<R<1\) and compare \(\lambda\) on the disc \(|z|<R\) with \(\mu_R(z)=\frac{2R}{R^2-|z|^2}\), the Poincaré metric of that disc, which also has curvature \(-1\) and tends to infinity at \(|z|=R\). The function \(u=\log(\lambda/\mu_R)\) tends to \(-\infty\) at the boundary, so if it is positive somewhere it has an interior maximum at a point with \(\lambda>0\). There \(\Delta u\le0\). But

\[ \Delta u=\Delta\log\lambda-\Delta\log\mu_R\ \ge\ \lambda^2-\mu_R^2>0, \]

using \(\Delta\log\lambda=-K_\lambda\lambda^2\ge\lambda^2\) and \(\Delta\log\mu_R=\mu_R^2\). Contradiction. So \(\lambda\le\mu_R\), and letting \(R\to1\) gives the result.

If \(f:\mathbb D\to\mathbb D\) is holomorphic, the pull-back \(\lambda=\lambda_{\mathbb D}(f(z))|f'(z)|\) has curvature \(-1\) where \(f'\ne0\). The lemma gives the Schwarz–Pick inequality \(\frac{|f'(z)|}{1-|f(z)|^2}\le\frac{1}{1-|z|^2}\).

Bloch’s constant

André Bloch proved that there is an absolute constant \(B>0\) such that every holomorphic \(f\) on \(\mathbb D\) with \(f'(0)=1\) maps some subdomain one-to-one onto a disc of radius \(B\). Applying his lemma to a cleverly built metric of curvature \(\le-1\), Ahlfors showed \(B\ge\sqrt3/4\approx0.433\). With Helmut Grunsky he had earlier shown \(B\le0.472\) and conjectured that this upper bound is exact. Despite many efforts the lower bound has been improved only in the fourth decimal place.

Exercise 6.1Verify that \(\lambda=\frac{2}{1-|z|^2}\) has curvature \(-1\). Use \(\Delta=4\partial_z\partial_{\bar z}\).

Show solution
\(\log\lambda=\log2-\log(1-z\bar z)\). Then \(\partial_{\bar z}\log\lambda=\frac{z}{1-z\bar z}\) and \(\partial_z\) of that is \(\frac{(1-z\bar z)+z\bar z}{(1-z\bar z)^2}=\frac{1}{(1-|z|^2)^2}\). So \(\Delta\log\lambda=\frac{4}{(1-|z|^2)^2}=\lambda^2\) and \(K=-1\).

Exercise 6.2Show that if \(\lambda\) has curvature \(\le-1\) and \(f\) is holomorphic, then the pull-back \(\lambda(f(z))|f'(z)|\) has curvature \(\le-1\) where \(f'\ne0\).

Show solution
\(\log(\lambda\circ f\cdot|f'|)=\log\lambda\circ f+\log|f'|\). The second term is harmonic where \(f'\ne0\). For the first, the chain rule for holomorphic \(f\) gives \(\Delta(\log\lambda\circ f)=(\Delta\log\lambda)\circ f\cdot|f'|^2\). So the curvature of the pull-back is \(-\frac{(\Delta\log\lambda)\circ f\,|f'|^2}{(\lambda\circ f)^2|f'|^2}=K_\lambda\circ f\le-1\).

Exercise 6.3Use Ahlfors’ lemma to prove Liouville’s theorem: a bounded entire function is constant.

Show solution
Suppose \(f:\mathbb C\to\mathbb D\) (after scaling). For each \(R\), \(g(z)=f(Rz)\) maps \(\mathbb D\) to \(\mathbb D\), so by Schwarz–Pick at \(0\), \(R|f'(0)|\le1-|f(0)|^2\le1\). Letting \(R\to\infty\) gives \(f'(0)=0\). The same argument at every point (translate first) gives \(f'\equiv0\).
Lesson 07

Extremal length and analytic capacity

For the general reader. How “wide” is a family of curves? Ahlfors and the Swedish analyst Arne Beurling answered with a number, the extremal length, that does not change under conformal maps. It became the universal tool for estimating conformal maps. In the same period Ahlfors asked which compact sets are too small to support a bounded analytic function, a question that was settled only in 2003.

Goals
  • Define extremal length and compute it for rectangles and annuli.
  • Define analytic capacity and Painlevé’s problem.

Let \(\Gamma\) be a family of locally rectifiable curves in a domain \(\Omega\). For a Borel function \(\rho\ge0\) on \(\Omega\), set \(L(\Gamma,\rho)=\inf_{\gamma\in\Gamma}\int_\gamma\rho\,|dz|\) and \(A(\rho)=\iint_\Omega\rho^2\,dx\,dy\).

Definition and invariance (Ahlfors–Beurling, 1950)

The extremal length of \(\Gamma\) is \(\lambda(\Gamma)=\sup_\rho\frac{L(\Gamma,\rho)^2}{A(\rho)}\), over \(\rho\) with \(0<A(\rho)<\infty\). If \(f:\Omega\to\Omega'\) is conformal, then \(\lambda(f(\Gamma))=\lambda(\Gamma)\). If \(f\) is \(K\)-quasiconformal, then \(K^{-1}\lambda(\Gamma)\le\lambda(f(\Gamma))\le K\lambda(\Gamma)\).

Invariance under conformal maps follows by transporting \(\rho\) to \(\rho\circ f^{-1}\,|(f^{-1})'|\), which preserves both lengths and area. The ideas were developed first independently by both men, then jointly in their 1950 paper in Acta Mathematica on conformal invariants and function-theoretic null-sets.

Analytic capacity

For a compact set \(E\subset\mathbb C\), let

\[ \gamma(E)=\sup\big\{|f'(\infty)| : f \text{ holomorphic on } \hat{\mathbb C}\setminus E,\ |f|\le1,\ f(\infty)=0\big\}, \]

where \(f'(\infty)=\lim_{z\to\infty}z\,f(z)\). A set is removable for bounded analytic functions exactly when \(\gamma(E)=0\). Ahlfors introduced \(\gamma\) in 1947 and proved that an extremal function exists and is unique; it is now called the Ahlfors function. Painlevé’s problem, to characterize removable sets geometrically, was solved through work of Guy David (1998) and Xavier Tolsa (2003), who showed that \(\gamma\) is comparable to a capacity defined by Menger curvature.

Exercise 7.1Let \(R=[0,a]\times[0,b]\) and \(\Gamma\) the curves in \(R\) joining the two vertical sides. Show \(\lambda(\Gamma)=a/b\).

Show solution
With \(\rho\equiv1\): \(L=a\), \(A=ab\), so \(\lambda\ge a^2/(ab)=a/b\). For any \(\rho\), each horizontal segment is in \(\Gamma\), so \(L\le\int_0^a\rho(x,y)dx\). Integrate in \(y\) and use Cauchy–Schwarz: \(bL\le\iint\rho\le(ab)^{1/2}A^{1/2}\). Hence \(L^2/A\le a/b\).

Exercise 7.2Let \(\Gamma\) be the curves joining the two boundary circles of the annulus \(r_1<|z|<r_2\). Show \(\lambda(\Gamma)=\frac{1}{2\pi}\log\frac{r_2}{r_1}\).

Show solution
Use \(\rho=1/|z|\): every curve has \(\int\rho|dz|\ge\int_{r_1}^{r_2}dr/r=\log(r_2/r_1)\), and \(A=2\pi\log(r_2/r_1)\), giving \(\lambda\ge\frac1{2\pi}\log\frac{r_2}{r_1}\). For the upper bound, take any \(\rho\). Each radial segment lies in \(\Gamma\), so \(L\le\int_{r_1}^{r_2}\rho\,dr\) for every angle. Integrating over the angle, \(2\pi L\le\iint\rho\,dr\,d\theta=\iint\frac{\rho}{r}\,dA\le A^{1/2}\big(2\pi\log\tfrac{r_2}{r_1}\big)^{1/2}\) by Cauchy–Schwarz. Squaring gives \(L^2/A\le\frac1{2\pi}\log\frac{r_2}{r_1}\).

Exercise 7.3Show that the analytic capacity of the closed disc \(|z|\le r\) is \(r\).

Show solution
\(f(z)=r/z\) is admissible with \(f'(\infty)=r\). Conversely, if \(f\) is admissible, then \(g(w)=f(r/w)\) is holomorphic on \(|w|<1\) with \(|g|\le1\), \(g(0)=0\), and \(g'(0)=f'(\infty)/r\). Schwarz’s lemma gives \(|g'(0)|\le1\), so \(|f'(\infty)|\le r\).
Lesson 08

Quasiconformal maps and the Beltrami equation

For the general reader. Teichmüller had shown, in papers few people read, that the best way to deform one Riemann surface into another stretches uniformly in one direction. After the war Ahlfors gave the theory solid foundations. With Lipman Bers he then proved that one can prescribe the infinitesimal stretching at every point, almost arbitrarily, and still find a map realizing it. This theorem underlies Teichmüller theory and complex dynamics.

Goals
  • Give Ahlfors’ geometric definition of quasiconformality.
  • State the measurable Riemann mapping theorem with holomorphic dependence.
  • Compute with the Beltrami equation.

A quadrilateral \(Q\) is a Jordan domain with four marked boundary points; its modulus \(\operatorname{mod}Q\) is the extremal length of the curves joining one pair of opposite sides, which equals \(a/b\) when \(Q\) is mapped conformally to an \(a\times b\) rectangle with vertices corresponding.

Definition (Ahlfors, 1953–54)

An orientation-preserving homeomorphism \(f\) of a plane domain is \(K\)-quasiconformal if \(\operatorname{mod}f(Q)\le K\operatorname{mod}Q\) for every quadrilateral \(Q\) in the domain.

This definition needs no differentiability. Ahlfors proved that such maps are differentiable almost everywhere and satisfy the Beltrami equation \(f_{\bar z}=\mu f_z\) with \(\|\mu\|_\infty\le\frac{K-1}{K+1}\). In the same 1953–54 paper he gave a complete proof of Teichmüller’s theorem on extremal maps between closed Riemann surfaces, using the length–area method in the metric of a quadratic differential.

Measurable Riemann mapping theorem (Ahlfors–Bers, 1960)

Let \(\mu\in L^\infty(\mathbb C)\) with \(\|\mu\|_\infty<1\). There is a unique quasiconformal homeomorphism \(f^\mu:\hat{\mathbb C}\to\hat{\mathbb C}\) fixing \(0,1,\infty\) with \(f^\mu_{\bar z}=\mu f^\mu_z\) almost everywhere. If \(\mu=\mu_t\) depends holomorphically on a complex parameter \(t\) (as an element of \(L^\infty\)), then \(f^{\mu_t}(z)\) is holomorphic in \(t\) for each \(z\).

Existence for measurable \(\mu\) goes back to Charles Morrey (1938). The Ahlfors–Bers contribution was a new proof through singular integrals, with the Beurling transform \(T\) whose \(L^p\) norms tend to 1 as \(p\to2\), and the holomorphic dependence on parameters, which is what Teichmüller theory and holomorphic dynamics need. Adrien Douady remarked at the 1986 Congress that before mating two polynomials one must first “Ahlfors–Bers” the structure.

Exercise 8.1Let \(\mu\) be constant with \(|\mu|<1\). Show that \(f(z)=z+\mu\bar z\) solves the Beltrami equation, and normalize it to fix \(0,1,\infty\).

Show solution
\(f_z=1\), \(f_{\bar z}=\mu\), so \(f_{\bar z}=\mu f_z\). It fixes 0 and \(\infty\) and sends 1 to \(1+\mu\). Divide: \(f^\mu(z)=\frac{z+\mu\bar z}{1+\mu}\), which has the same Beltrami coefficient.

Exercise 8.2If \(f\) has Beltrami coefficient \(\mu\) and \(h\) is conformal, show that \(h\circ f\) has coefficient \(\mu\), and \(f\circ h\) has coefficient \((\mu\circ h)\,\overline{h'}/h'\).

Show solution
\((h\circ f)_z=h'(f)f_z\) and \((h\circ f)_{\bar z}=h'(f)f_{\bar z}\), so the ratio is \(\mu\). For \(f\circ h\): \((f\circ h)_z=f_z(h)h'\) and \((f\circ h)_{\bar z}=f_{\bar z}(h)\overline{h'}\). The ratio is \(\mu(h)\overline{h'}/h'\). This is why Beltrami coefficients on a Riemann surface are \((-1,1)\)-forms.

Exercise 8.3Let \(\mu_t=t\nu\) with \(\nu\in L^\infty\), \(\|\nu\|_\infty\le1\), and \(|t|<1\). For \(\nu\) constant, check directly that \(f^{\mu_t}(z)\) is holomorphic in \(t\).

Show solution
From 8.1, \(f^{t\nu}(z)=\frac{z+t\nu\bar z}{1+t\nu}\). For fixed \(z\) this is a rational function of \(t\) with its pole at \(t=-1/\nu\), outside \(|t|<1\). So it is holomorphic in \(t\).
Lesson 09

Quasicircles and universal Teichmüller space

For the general reader. Which closed curves are images of a circle under a quasiconformal map of the plane? In 1963 Ahlfors gave a strikingly simple answer: a curve qualifies exactly when it does not double back on itself too sharply, a condition on any three of its points. The same paper showed that the space of all such shapes is an open set in a space of holomorphic functions, the universal Teichmüller space of Bers.

Goals
  • State Ahlfors’ three-point condition.
  • Relate quasisymmetric boundary maps to quasiconformal extensions.

A quasicircle is the image of the unit circle under a quasiconformal homeomorphism of \(\hat{\mathbb C}\).

Theorem (Ahlfors, 1963)

A Jordan curve \(C\subset\mathbb C\) is a quasicircle if and only if there is a constant \(M\) such that for any two points \(z_1,z_2\in C\) and any \(z_3\) on the smaller-diameter arc of \(C\) between them,

\[ |z_1-z_3|+|z_3-z_2|\le M\,|z_1-z_2| . \]

The proof builds a quasiconformal reflection across \(C\): an orientation-reversing quasiconformal map of the sphere that fixes \(C\) pointwise and swaps its two sides. Its existence is equivalent to \(C\) being a quasicircle.

Boundary values

In 1956 Beurling and Ahlfors characterized the boundary values of quasiconformal self-maps of the upper half-plane: an increasing homeomorphism \(h\) of \(\mathbb R\) extends to a quasiconformal map of \(\mathbb H\) if and only if it is quasisymmetric, meaning

\[ \frac1M\le\frac{h(x+t)-h(x)}{h(x)-h(x-t)}\le M\quad\text{for all }x\in\mathbb R,\ t>0 . \]

Their extension formula is explicit. They also showed that such \(h\) can be singular with respect to Lebesgue measure. The space of quasisymmetric maps modulo Möbius maps is the universal Teichmüller space, which contains the Teichmüller space of every Riemann surface. Ahlfors’ 1963 paper showed that its image under the Schwarzian derivative is open in the Banach space of bounded holomorphic quadratic differentials on the half-plane.

Exercise 9.1Show that the boundary of the square \([0,1]^2\) satisfies the three-point condition, and find a valid constant \(M\).

Show solution
If \(z_1,z_2\) are on the same side or adjacent sides, the arc between them is a segment or an L-shaped path, and for \(z_3\) on it, \(|z_1-z_3|+|z_3-z_2|\) is at most the arc length, which is at most \(\sqrt2|z_1-z_2|\) for an L with a right angle. If they are on opposite sides, then \(|z_1-z_2|\ge1\), and the smaller-diameter arc has diameter at most \(\sqrt2\), so the sum is at most \(2\sqrt2\le2\sqrt2|z_1-z_2|\). So \(M=2\sqrt2\) works.

Exercise 9.2Show that the boundary of the cusp region \(\{x+iy:0<x<1,\ |y|<x^2\}\) is not a quasicircle.

Show solution
Take \(z_1=t+it^2\), \(z_2=t-it^2\) for small \(t\). The smaller arc between them passes through the cusp at 0, so take \(z_3=0\). Then \(|z_1-z_3|+|z_3-z_2|\approx2t\) while \(|z_1-z_2|=2t^2\). The ratio \(1/t\) is unbounded.

Exercise 9.3Show that \(h(x)=x|x|^{\alpha-1}\) with \(\alpha>0\) is quasisymmetric on \(\mathbb R\).

Show solution
\(h\) is an increasing homeomorphism commuting with dilations: \(h(sx)=s^\alpha h(x)\) for \(s>0\). So the ratio depends only on \(u=x/t\). As a continuous positive function of \(u\in\mathbb R\), it tends to 1 as \(u\to\pm\infty\) (where \(h\) is nearly linear over the interval), and so it is bounded above and below. (At \(u=0\) the ratio is exactly 1 by oddness.)
Lesson 10

Kleinian groups: finiteness and measure

For the general reader. A Kleinian group is a discrete group of Möbius transformations of the sphere. Where the group acts nicely, the quotient is a collection of Riemann surfaces. In 1964 Ahlfors proved that a group with finitely many generators produces only finitely many surfaces, each of finite type. He also posed a problem about the leftover “limit set” that took forty years to solve.

Goals
  • Define the limit set and the region of discontinuity.
  • State Ahlfors’ finiteness theorem and the Bers area inequality.
  • Know the fate of the measure conjecture.

Let \(\Gamma\subset\mathrm{PSL}_2(\mathbb C)\) be a discrete group acting on \(\hat{\mathbb C}\). Its region of discontinuity \(\Omega(\Gamma)\) is the set of points with a neighbourhood \(U\) such that \(\gamma U\cap U\ne\varnothing\) for only finitely many \(\gamma\). The complement \(\Lambda(\Gamma)\) is the limit set. The group is Kleinian if \(\Omega\ne\varnothing\).

Ahlfors finiteness theorem (1964)

If \(\Gamma\) is a finitely generated Kleinian group, then \(\Omega(\Gamma)/\Gamma\) is a finite union of Riemann surfaces, each a closed surface with finitely many punctures and finitely many cone points.

Ahlfors proved this with Eichler cohomology and quasiconformal deformations: each component of the quotient contributes independently to a space of deformations of \(\Gamma\), which is finite-dimensional because \(\Gamma\) is finitely generated. A gap concerning thrice-punctured spheres was closed by later work of Bers, Leon Greenberg and Ahlfors. In 1967 Bers proved a quantitative version: if \(\Gamma\) is generated by \(N\ge2\) elements, the total hyperbolic area of \(\Omega/\Gamma\) is at most \(4\pi(N-1)\).

Ahlfors measure conjecture (mid-1960s)

If \(\Gamma\) is a finitely generated Kleinian group, then \(\Lambda(\Gamma)\) either is all of \(\hat{\mathbb C}\) or has two-dimensional Lebesgue measure zero.

Ahlfors proved it for geometrically finite groups. Dennis Sullivan proved around 1980 that the limit set supports no invariant line field, the analytic statement Ahlfors’ question was really about. The full conjecture followed from the tameness theorem, proved in 2004 by Ian Agol and independently by Danny Calegari and David Gabai, combined with earlier work of Richard Canary. William Thurston’s geometrization of 3-manifolds had in the meantime shown that Kleinian groups are the same subject as hyperbolic 3-manifolds.

Exercise 10.1A Schottky group of rank \(N\) is generated by \(N\) Möbius maps \(g_i\), each sending the outside of a circle \(C_i\) onto the inside of a circle \(C_i'\), with all \(2N\) circles disjoint. Its quotient \(\Omega/\Gamma\) is a closed surface of genus \(N\). Show that it attains the Bers bound.

Show solution
By Gauss–Bonnet, a closed hyperbolic surface of genus \(N\) has area \(-2\pi\chi=2\pi(2N-2)=4\pi(N-1)\). The group needs exactly \(N\) generators, so the bound \(4\pi(N-1)\) is attained.

Exercise 10.2For the cyclic group generated by \(z\mapsto2z\), find \(\Lambda\), \(\Omega\) and \(\Omega/\Gamma\).

Show solution
Orbits accumulate only at \(0\) and \(\infty\), so \(\Lambda=\{0,\infty\}\) and \(\Omega=\mathbb C^\times\). The quotient \(\mathbb C^\times/\langle z\mapsto2z\rangle\) is a torus: via \(z=e^w\) it is \(\mathbb C/(\log2\,\mathbb Z+2\pi i\mathbb Z)\). One surface of finite type, as the finiteness theorem predicts, and \(\Lambda\) has measure zero.

Exercise 10.3Compute the image of the circle \(|z-c|=r\) under inversion in the circle \(|z-a|=R\), assuming \(|c-a|\ne r\). (This is the formula used to draw the picture at the top of this page.)

Show solution
Inversion is \(z\mapsto a+\frac{R^2}{\overline{z-a}}\). Let \(d=|c-a|\) and \(s=\frac{R^2}{d^2-r^2}\). The image is the circle with centre \(a+s(c-a)\) and radius \(|s|\,r\). Check on the two points of the circle on the line through \(a\) and \(c\): they lie at distances \(d\pm r\) from \(a\) and go to distances \(R^2/(d\pm r)\), whose midpoint is \(R^2d/(d^2-r^2)=sd\) and half-difference is \(R^2r/|d^2-r^2|=|s|r\).
Part III · Life and legacy
Lesson 11

War, Zürich, Harvard, 1938–1977

Ahlfors returned to Helsinki in 1938. The Winter War with the Soviet Union began in November 1939, and the Continuation War followed in 1941, with Finland fighting alongside Germany. Helsinki was bombed, and the university nearly emptied because the male students were at the front. Ahlfors was exempt from military service because of an earlier medical condition. He sent his wife and children to safety in Sweden and kept teaching. He later recalled writing one of his best papers in an air-raid shelter.

Finland signed an armistice with the Soviet Union in September 1944. In the spring of 1945 Ahlfors took up a professorship in Zürich, reaching it after a difficult journey across a disrupted continent; MacTutor reports that he pawned his Fields Medal to help pay for the trip out of Finland. He was not happy in Zürich, and in 1946 he accepted Harvard’s offer to return. He stayed for the rest of his career, chaired the department, became William Caspar Graustein Professor in 1964 and retired in 1977.

At Harvard his research entered its second great period. Lipman Bers, at Syracuse, Princeton and then Columbia, became his closest mathematical partner. Their joint seminar culture, and the regular conferences on Riemann surfaces and Kleinian groups that began in the 1960s, created the school from which Teichmüller theory, Kleinian groups and holomorphic dynamics grew. He also read and championed Teichmüller’s work and, with Frederick Gehring, edited Teichmüller’s collected papers in 1982.

Lesson 12

Teacher, author, legacy

Ahlfors supervised 24 doctoral students and many postdoctoral visitors. They include Paul Garabedian, James Jenkins, George Springer, Halsey Royden, Robert Osserman, Clifford Earle, Albert Marden, Henry Pollak and Dale Husemoller. Royden proved that the Teichmüller metric equals the Kobayashi metric; Earle and Marden became leaders of Teichmüller and Kleinian group theory.

Books

  • Complex Analysis (1953; 3rd ed. 1979), the classic graduate text, admired for its economy and precision.
  • Riemann Surfaces, with Leo Sario (1960).
  • Lectures on Quasiconformal Mappings (1966), the short book from which most of the field learned the subject.
  • Conformal Invariants: Topics in Geometric Function Theory (1973).
  • Möbius Transformations in Several Dimensions (1981).

Honours

Ahlfors received the Fields Medal (1936), the Wihuri International Prize (1968), the Wolf Prize (1981, shared with Oscar Zariski) and the Steele Prize of the American Mathematical Society (1982). He was a member of the US National Academy of Sciences and of several European academies, and honorary president of the 1986 International Congress in Berkeley. The Wolf Prize jury said that every complex analyst is in some sense his student. His Collected Papers appeared in two volumes in 1982.

He remained mathematically active long after retirement. He died on 11 October 1996 in Pittsfield, Massachusetts, at the age of 89, survived by his wife Erna and their three daughters.

Influence

  • Value distribution: the geometric theory of covering surfaces and the five islands theorem, now used in complex dynamics and in the study of normal families.
  • Geometry of curvature: Ahlfors’ lemma is the prototype of the Schwarz lemmas of Shiing-Shen Chern, Shing-Tung Yau and Shoshichi Kobayashi.
  • Quasiconformal maps: the Ahlfors–Bers theorem drives Teichmüller theory and holomorphic dynamics, from Douady and Hubbard to Curtis McMullen.
  • Kleinian groups: the finiteness theorem and the measure conjecture shaped the field that Thurston connected to 3-manifold topology.

DiscussionAhlfors spent the war in a country allied with Germany, then built at Harvard, with the refugee Lipman Bers, the theory founded by the Nazi activist Teichmüller. How did mathematicians of that generation separate, or fail to separate, ideas from their authors? Compare with the Teichmüller module of this series.

Final projectChoose one theorem from Part II. Write a two-page account for a strong undergraduate that states it, works one example in full, and explains which earlier result it made geometric.

Reference

Connections

People linked to Lars Ahlfors across this collection. A name without a link has no page here yet. See Lars Ahlfors in the network of all 337 lives →

Teachers and advisors

  • Ernst Lindelöf 1924-1930
  • Rolf Nevanlinna 1924-1930

Students

  • Albert Marden
  • Clifford Earle 1962
  • George Springer
  • Halsey Royden
  • James A. Jenkins
  • Paul Garabedian
  • Robert Osserman

Influenced by

Influenced

Colleagues and collaborators

  • Oscar Zariski 1981
  • Arne Beurling 1946-1956
  • Constantin Carathéodory
  • Frederick Gehring
  • Lipman Bers 1950s-1970s

Also mentioned in this life

Fields

On CoursesHub

Reference

Sources and further reading

Biography

  1. J. J. O’Connor and E. F. Robertson, Lars Valerian Ahlfors, MacTutor History of Mathematics.
  2. F. W. Gehring, Lars Valerian Ahlfors 1907–1996, Biographical Memoirs of the National Academy of Sciences 87 (2005).
  3. Lars Ahlfors, Wikipedia.
  4. Mathematics Genealogy Project (entry for C. J. Earle, Ahlfors’ student).
  5. L. V. Ahlfors, Collected Papers, 2 vols., Birkhäuser, 1982 (with his own commentaries).

Mathematics

  1. L. V. Ahlfors, Zur Theorie der Überlagerungsflächen, Acta Math. 65 (1935).
  2. L. V. Ahlfors, An extension of Schwarz’s lemma, Trans. AMS 43 (1938).
  3. L. V. Ahlfors, Bounded analytic functions, Duke Math. J. 14 (1947).
  4. L. V. Ahlfors and A. Beurling, Conformal invariants and function-theoretic null-sets, Acta Math. 83 (1950).
  5. L. V. Ahlfors, On quasiconformal mappings, J. Analyse Math. 3 (1953–54).
  6. A. Beurling and L. V. Ahlfors, The boundary correspondence under quasiconformal mappings, Acta Math. 96 (1956).
  7. L. V. Ahlfors and L. Bers, Riemann’s mapping theorem for variable metrics, Ann. of Math. 72 (1960).
  8. L. V. Ahlfors, Quasiconformal reflections, Acta Math. 109 (1963).
  9. L. V. Ahlfors, Finitely generated Kleinian groups, Amer. J. Math. 86 (1964).
  10. L. V. Ahlfors, Lectures on Quasiconformal Mappings, 2nd ed., AMS, 2006.
  11. L. V. Ahlfors, Conformal Invariants, McGraw-Hill, 1973; reprinted AMS Chelsea, 2010.
  12. W. K. Hayman, Meromorphic Functions, Oxford, 1964 (Ahlfors’ theory of covering surfaces, chapter 5).
  13. J. B. Garnett and D. E. Marshall, Harmonic Measure, Cambridge, 2005 (extremal length and the distortion theorem).