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Discrete Holomorphic Local Dynamical Systems

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

Consider the second case with multi-indices i ∈ I. Letqdenote the integer part<br />

of λ n and Wα the projection of Γn ∩ Uα on Pk by Π0. Observe that the choice of the<br />

open sets Ui implies that f q is injective on Wα. Therefore,<br />

∑ α<br />

�<br />

Γn∩Uα<br />

≤ ∑<br />

α Wα<br />

�<br />

= ∑<br />

α<br />

�<br />

≤ ∑ α<br />

Π ∗<br />

i1 (ωFS) ∧ ...∧ Π ∗<br />

i (ωFS)<br />

k<br />

�<br />

( f i1 ∗<br />

) (ωFS) ∧ ...∧ ( f ik ∗<br />

) (ωFS)<br />

Wα<br />

( f q ) ∗� ( f i1−q ) ∗ (ωFS) ∧ ...∧ ( f i k−q ) ∗ (ωFS) �<br />

P k( f i1−q ) ∗ (ωFS) ∧ ...∧ ( f i k−q ) ∗ (ωFS).<br />

Recall that the number of open sets Uα is bounded by d kρn . So, the last sum is<br />

bounded by<br />

d kρn d (i1−q)+···+(i k−q) ≤ d kρn d k(n−q) � d k(1+ρ−λ )n .<br />

Finally, since the number of multi-indices i is less than n k , we deduce from the<br />

above estimates that<br />

k!volume(Γn ∩ Vn) � n k d (k−1+λ )n + n k d k(1+ρ−λ )n .<br />

This contradicts the above bound from below of volume(Γn ∩ Vn). ⊓⊔<br />

The remaining part of this paragraph deals with Lyapounov exponents associated<br />

to the measure μ and their relations with the Hausdorff dimension of μ. Results<br />

in this direction give some information about the rough geometrical behaviour of<br />

the dynamical system on the most chaotic locus. An abstract theory was developed<br />

by Oseledec and Pesin, see e.g. [KH]. However, it is often difficult to show that<br />

a given dynamical system has non-vanishing Lyapounov exponents. In complex<br />

dynamics as we will see, the use of holomorphicity makes the goal reachable. We<br />

first introduce few notions.<br />

Let A be a linear endomorphism of R k . We can write R k as the direct sum ⊕Ei<br />

of invariant subspaces on which all the complex eigenvalues of A have the same<br />

modulus. This decomposition of R k describes clearly the geometrical behaviour of<br />

the dynamical system associated to A. An important part in the dynamical study<br />

with respect to an invariant measure is to describe geometrical aspects following<br />

the directional dilation or contraction indicators.<br />

Consider a smooth dynamical system g : X → X and an invariant ergodic probability<br />

measure ν. Themapg induces a linear map from the tangent space at x to<br />

the tangent space at g(x). This linear map is given by a square matrix when we fix<br />

local coordinates near x and g(x). Then, we obtain a function on X with values in<br />

GL(R,k) where k denotes the real dimension of X. We will study the sequence of<br />

such functions associated to the sequence of iterates (g n ) of g.

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