Douady–Earle extension

In mathematics, the Douady–Earle extension, named after Adrien Douady and Clifford Earle, is a way of extending homeomorphisms of the unit circle in the complex plane to homeomorphisms of the closed unit disk, such that the extension is a diffeomorphism of the open disk. The extension is analytic on the open disk. The extension has an important equivariance property: if the homeomorphism is composed on either side with a Möbius transformation preserving the unit circle the extension is also obtained by composition with the same Möbius transformation. If the homeomorphism is quasisymmetric, the diffeomorphism is quasiconformal. An extension for quasisymmetric homeomorphisms had previously been given by Ahlfors and Arne Beurling; a different equivariant construction had been given in 1985 by Pekka Tukia. Equivariant extensions have important applications in Teichmüller theory, for example they lead to a quick proof of the contractibility of the Teichmüller space of a Fuchsian group.

Definition

By the Radó–Kneser–Choquet theorem, the Poisson integral Ff of a homeomorphism f of the circle defines a harmonic diffeomorphism of the unit disk extending f. If f is quasisymmetric, the extension is not necessarily quasiconformal, i.e. the complex dilatation

\displaystyle{\mu(z)={\partial_{\overline{z}}F_f\over \partial_z F_f},}

does not necessarily satisfy

\displaystyle{\sup_{|z|<1} |\mu(z)| < 1.}

However F can be used to define another analytic extension Hf of f−1 which does satisfy this condition. It follows that

\displaystyle{E(f)=H_{f^{-1}}}

is the required extension.

For |a| < 1 define the Möbius transformation

\displaystyle{g_a(z)= {z-a\over 1- \overline{a}z}.}

It preserves the unit circle and unit disk sending a to 0.

If g is any Möbius transformation preserving the unit circle and disk, then

\displaystyle{F_{f\circ g} = F_f\circ g.}

For |a| < 1 define

\displaystyle{w=H_f(a)}

to be the unique w with |w| < 1 and

\displaystyle{F_{g_a\circ f}(w) =0.}

For |a| =1 set

\displaystyle{H_f(a)=f^{-1}(a).}

Properties

\displaystyle{H_{g\circ f \circ h} = h^{-1}\circ H_f \circ g^{-1}}
for any Möbius transformations g and h preserving the unit circle and disk.
\displaystyle{\Phi(a,b)= F_{g_a\circ f}(b)={1\over 2\pi}\int_0^{2\pi} g_a\circ f\circ g_{-b}(e^{i\theta})\, d\theta={1\over 2\pi}\int_0^{2\pi} \left({f(e^{i\theta}) -b\over 1-\overline{b}f(e^{i\theta})}\right) {1-|a|^2\over |a-e^{i\theta}|^2}\, d\theta}
If zn and wn lie in the unit disk and tend to z and w and homeomorphisms of the circle are defined by
\displaystyle{f_n=g_{z_n}\circ f \circ g_{-w_n},}
then fn tends almost everywhere to
By the dominated convergence theorem, it follows that Φ(zn,wn) has a non-zero limit if wHf(z). This implies that Hf is continuous on the closed unit disk. Indeed otherwise, by compactness, there would be a sequence zn tending to z in the closed disk, with wn = Hf(zn) tending to a limit wHf(z). But then Φ(zn,wn) = 0 so has limit zero, a contradiction, since wHf(z).
If f has Fourier series
\displaystyle{f(e^{i\theta}) = \sum_m a_m e^{im\theta},}
then the derivatives of Ff at 0 are given by
\displaystyle{\partial_z F_f (0)= a_{1},\,\,\, \partial_{\overline{z}} F_f(0) =a_{-1}.}
Thus the Jacobian of Ff at 0 is given by
  \displaystyle{|\partial_z F_f(0)|^2 -  |\partial_{\overline{z}} F_f(0)|^2 = |a_{1}|^2 - |a_{-1}|^2.}
Since Ff is an orientation-preserving diffeomorphism, its Jacobian is positive:
\displaystyle{|a_{1}|^2 - |a_{-1}|^2 >0.}
The function Φ(z,w) is analytic and so smooth. Its derivatives at (0,0) are given by
\displaystyle{\Phi_z(0,0)=a_{-1},\,\,\Phi_{\overline{z}}(0,0)=a_{1},\,\, \Phi_{w}(0,0) = -1,\,\, \Phi_{\overline{w}}(0,0) = {1\over 2\pi} \int_0^{2\pi} f(e^{i\theta})^2\, d\theta=b.}
Direct calculation shows that
\displaystyle{|\Phi_{w}(0,0)|^2 - |\Phi_{\overline{w}}(0,0)|^2=1-\left|{1\over 2\pi}\int_0^{2\pi} f(e^{i\theta})^2 \, d\theta\right|^2 \ge 0.}
by the Cauchy–Schwarz inequality. If the right hand side vanished, then equality would occur in the Cauchy-Schwarz inequality forcing
\displaystyle{f(e^{i\theta}) =\zeta \overline{f(e^{i\theta})}}
for some ζ in T and for all θ, a contradiction since f assumes all values in T. The left hand side is therefore strictly positive and |b| < 1.
Consequently the implicit function theorem can be applied. It implies that Hf(z) is smooth near o. Its Jacobian can be computed by implicit differentiation:
\displaystyle{|\partial_z H_f(0)|^2 -  |\partial_{\overline{z}}H_f(0)|^2 = {|\Phi_z(0,0)|^2 - |\Phi_{\overline{z}}(0,0)|^2 \over |\Phi_w(0,0)|^2 -|\Phi_{\overline{w}}(0,0)|^2} >0.}
Moreover
\displaystyle{{\partial_{\overline{z}}H_f (0)\over \partial_{z} H_f(0)}=g_b\left(-{a_{-1}\over \overline{a_{1}}}\right).}

Extension of quasi-Möbius homeomorphisms

In this section it is established that the extension of a quasisymmetric homeomorphism is quasiconformal. Fundamental use is made of the notion of quasi-Möbius homeomorphism.

A homeomorphism f of the circle is quasisymmetric if there are constants a, b > 0 such that

\displaystyle{{|f(z_1)-f(z_2)|\over |f(z_1)-f(z_3)|} \le a {|z_1-z_2|^b\over |z_1-z_3|^b}.}

It is quasi-Möbius is there are constants c, d > 0 such that

\displaystyle{|(f(z_1),f(z_2);f(z_3),f(z_4))| \le c |(z_1,z_2;z_3,z_4)|^d,}

where

\displaystyle{ (z_1,z_2;z_3,z_4)={(z_1-z_3)(z_2-z_4)\over(z_2-z_3)(z_1-z_4)}}

denotes the cross-ratio.

If f is quasisymmetric then it is also quasi-Möbius, with c = a2 and d = b: this follows by multiplying the first inequality for (z1,z3,z4) and (z2,z4,z3). (Conversely Väisäläa (1985) has shown that a quasi-Möbius homeomorphism is also quasisymmetric.)

It is immediate that the quasi-Möbius homeomorphisms are closed under the operations of inversion and composition.

The complex dilatation μ of a diffeomorphism F of the unit disk is defined by

\displaystyle{\mu_F(z)={\partial_{\overline{z}}F(z)\over \partial_z F(z)}.}

If F and G are diffeomorphisms of the disk, then

\displaystyle{\mu_{G\circ F^{-1}}\circ F={F_z\over \overline{F_z}} {\mu_G-\mu_F\over 1 -\overline{\mu_F}\mu_G}.}

In particular if G is holomorphic, then

\displaystyle{\mu_{F\circ G^{-1}} \circ G = {G_z\over \overline{G_z}} \mu_F,\,\,\, \mu_{G^{-1}\circ F}=\mu_F.}

When F = Hf,

\displaystyle{\mu_F(0)=g_b\left( -{a_{-1}\over \overline{a_{1}}}\right),}

where

\displaystyle{a_{\pm 1}={1\over 2\pi} \int_0^{2\pi} f(e^{i\theta})e^{\mp i\theta} \, d\theta,\,\,\, b={1\over 2\pi} \int_0^{2\pi} f(e^{i\theta})^2 \, d\theta.}

To prove that F = Hf is quasiconformal amounts to showing that

\displaystyle{\|\mu_F\|_\infty < 1.}

Since f ia a quasi-Möbius homeomorphism the compositions g1fg2 with gi Möbius transformations satisfy exactly the same estimates, since Möbius transformations preserve the cross ratio. So to prove that Hf is quasiconformal it suffices to show that if f is any quasi-Möbius homeomorphism fixing 1, i and −i, with fixed c and d, then the quantities

\displaystyle{\Lambda(f)=\left|g_b\left( -{a_{-1}\over \overline{a_{1}}}\right)\right|}

have an upper bound strictly less than one.

On the other hand if f is quasi-Möbius and fixes 1, i and −i, then f satisfies a Hölder continuity condition:

\displaystyle{|f(z)-f(w)|\le C |z-w|^d,}

for another positive constant C independent of f. The same is true for the f−1's. But then the Arzelà–Ascoli theorem implies these homeomorphisms form a compact subset in C(T). The non-linear functional Λ is continuous on this subset and therefore attains its upper bound at some f0. On the other hand Λ(f0) < 1, so the upper bound is strictly less than 1.

The uniform Hölder estimate for f is established in Väisäläa (1985) as follows. Take z, w in T.

\displaystyle{|(w,i; z,-i)| \le 16|z-w|,\,\,\, |(f(w),i; f(z),-i)| \ge  |f(z)-f(w)|/8,}
so there is a corresponding Hölder estimate.
\displaystyle{ |(z,\zeta;w,1)| \le 8|z-w|,\,\,\, |(f(z),\zeta; f(w),1)|\ge  |f(z)-f(w)|/8,}
so there is a corresponding Hölder estimate.

References

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