Koenigs function explained

In mathematics, the Koenigs function is a function arising in complex analysis and dynamical systems. Introduced in 1884 by the French mathematician Gabriel Koenigs, it gives a canonical representation as dilations of a univalent holomorphic mapping, or a semigroup of mappings, of the unit disk in the complex numbers into itself.

Existence and uniqueness of Koenigs function

Let D be the unit disk in the complex numbers. Let be a holomorphic function mapping D into itself, fixing the point 0, with not identically 0 and not an automorphism of D, i.e. a Möbius transformation defined by a matrix in SU(1,1).

By the Denjoy-Wolff theorem, leaves invariant each disk |z | < r and the iterates of converge uniformly on compacta to 0: in fact for 0 < < 1,

|f(z)|\leM(r)|z|

for |z | ≤ r with M(r) < 1. Moreover '(0) = with 0 < || < 1.

proved that there is a unique holomorphic function h defined on D, called the Koenigs function, such that (0) = 0, '(0) = 1 and Schröder's equation is satisfied,

h(f(z))=f\prime(0)h(z)~.

The function h is the uniform limit on compacta of the normalized iterates,

gn(z)=λ-nfn(z)

.

Moreover, if is univalent, so is .

As a consequence, when (and hence) are univalent, can be identified with the open domain . Under this conformal identification, the mapping   becomes multiplication by, a dilation on .

Proof

H=k\circh-1(z)

near 0. Thus H(0) =0, H(0)=1 and, for |z | small,

λH(z)h(k-1(z))=h(f(k-1(z))=h(k-1(λz)=H(λz)~.

Substituting into the power series for, it follows that near 0. Hence near 0.

F(z)=f(z)/λz,

then by the Schwarz lemma

|F(z)-1|\le(1+|λ|-1)|z|~.

On the other hand,

gn(z)=

n-1
z\prod
j=0

F(fj(z))~.

Hence gn converges uniformly for |z| ≤ r by the Weierstrass M-test since

\sum\sup|z|\le|1-F\circfj(z)|\le(1+|λ|-1)\sumM(r)j<infty.

Koenigs function of a semigroup

Let be a semigroup of holomorphic univalent mappings of into itself fixing 0 defined for such that

fs

is not an automorphism for > 0

fs(ft(z))=ft+s(z)

f0(z)=z

ft(z)

is jointly continuous in and

Each with > 0 has the same Koenigs function, cf. iterated function. In fact, if h is the Koenigs function of, then satisfies Schroeder's equation and hence is proportion to h.

Taking derivatives gives

h(fs(z))

\prime(0)
=f
s

h(z).

Hence is the Koenigs function of .

Structure of univalent semigroups

On the domain, the maps become multiplication by

\prime(0)
λ(s)=f
s
, a continuous semigroup.So

λ(s)=e\mu

where is a uniquely determined solution of with Re < 0. It follows that the semigroup is differentiable at 0. Let

v(z)=\partialtft(z)|t=0,

a holomorphic function on with v(0) = 0 and = .

Then

\partialt(ft(z))

\prime(f
h
t(z))=

\mue\muh(z)=\muh(ft(z)),

so that

v=v\prime(0){h\overh\prime}

and

\partialtft(z)=v(ft(z)),ft(z)=0~,

the flow equation for a vector field.

Restricting to the case with 0 < λ < 1, the h(D) must be starlike so that

\Re{zh\prime(z)\overh(z)}\ge0~.

Since the same result holds for the reciprocal,

\Re{v(z)\overz}\le0~,

so that satisfies the conditions of

v(z)=zp(z),\Rep(z)\le0,p\prime(0)<0.

Conversely, reversing the above steps, any holomorphic vector field satisfying these conditions is associated to a semigroup, with

h(z)=z\exp

z
\int
0

{v\prime(0)\overv(w)}-{1\overw}dw.

References

. Functional equations in a single variable . Marek Kuczma. Monografie Matematyczne . 1968 . PWN – Polish Scientific Publishers . Warszawa. ASIN: B0006BTAC2