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Discrete Holomorphic Local Dynamical Systems

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222 Tien-Cuong Dinh and Nessim Sibony<br />

Exercise 1.104. Show that if a Borel set A satisfies μ(A) > 0, then μ( f n (A))<br />

converges to 1.<br />

Exercise 1.105. Show that sup ψ In(ϕ,ψ) with ψ smooth �ψ�∞ ≤ 1 is equal to<br />

�ϕ� L 1 (μ) . Deduce that there is no decay of correlations which is uniform on �ψ�∞.<br />

Exercise 1.106. Let V1 := {ψ ∈ L 2 0 (μ), Λ(ψ) =0}. Show that V1 is infinite<br />

dimensional and that bounded functions in V1 are dense in V1 with respect to<br />

the L 2 (μ)-topology. Using Theorem 1.82, show that the only eigenvalues of Λ are<br />

0 and 1.<br />

Exercise 1.107. Let ϕ be a d.s.h. function as in Corollary 1.88. Show that<br />

�ϕ + ···+ ϕ ◦ f n−1 � 2<br />

L 2 (μ) − nσ 2 + γ = O(d −n ),<br />

where γ := 2∑n≥1 n〈μ,ϕ(ϕ ◦ f n )〉 is a finite constant. Prove an analogous property<br />

for ϕ Hölder continuous.<br />

1.7 Entropy, Hyperbolicity and Dimension<br />

There are various ways to describe the complexity of a dynamical system. A basic<br />

measurement is the entropy which is closely related to the volume growth of the<br />

images of subvarieties. We will compute the topological entropy and the metric entropy<br />

of holomorphic endomorphisms of P k . We will also estimate the Lyapounov<br />

exponents with respect to the measure of maximal entropy and the Hausdorff<br />

dimension of this measure.<br />

We recall few notions. Let (X,dist) be a compact metric space where dist is a<br />

distance on X. Letg : X → X be a continuous map. We introduce the Bowen metric<br />

associated to g. For a positive integer n, define the distance distn on X by<br />

distn(x,y) := sup<br />

0≤i≤n−1<br />

dist(g i (x),g i (y)).<br />

We have distn(x,y) > ε if the orbits x,g(x),g 2 (x),... of x and y,g(y),g 2 (y),... of y<br />

are distant by more than ε at a time i less than n. In which case, we say that x,y are<br />

(n,ε)-separated.<br />

The topological entropy measures the rate of growth in function of time n, of<br />

the number of orbits that can be distinguished at ε-resolution. In other words, it<br />

measures the divergence of the orbits. More precisely, for K ⊂ X, not necessarily invariant,<br />

let N(K,n,ε) denote the maximal number of points in K which are pairwise<br />

(n,ε)-separated. This number increases as ε decreases. The topological entropy of<br />

g on K is<br />

1<br />

ht(g,K) := suplimsup<br />

ε>0 n→∞ n logN(K,n,ε).

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