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.
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|
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 .
H=k\circh-1(z)
near 0. Thus H(0) =0, H(0)=1 and, for |z | small,
λH(z)=λh(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,
|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.
Let be a semigroup of holomorphic univalent mappings of into itself fixing 0 defined for such that
fs
fs(ft(z))=ft+s(z)
f0(z)=z
ft(z)
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).
On the domain, the maps become multiplication by
\prime(0) | |
λ(s)=f | |
s |
λ(s)=e\mu
v(z)=\partialtft(z)|t=0,
Then
\partialt(ft(z))
\prime(f | |
h | |
t(z))= |
\mue\muh(z)=\muh(ft(z)),
v=v\prime(0){h\overh\prime}
\partialtft(z)=v(ft(z)),ft(z)=0~,
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~,
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.
. Functional equations in a single variable . Marek Kuczma. Monografie Matematyczne . 1968 . PWN – Polish Scientific Publishers . Warszawa. ASIN: B0006BTAC2