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Discrete Holomorphic Local Dynamical Systems

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

If g is the Green function of f ,wehave<br />

( f n1 ) ∗ (ωFS)=d n1 T − dd c (g ◦ f n1 ).<br />

The above integral is equal to the sum of the following integrals<br />

d n1<br />

�<br />

T p−r+1 ∧ ( f n2 ∗<br />

) (ωFS) ∧ ...∧ ( f ns ∗<br />

) (ωFS) ∧ χω k−p+r−s<br />

FS<br />

and<br />

�<br />

−<br />

T p−r ∧ dd c (g ◦ f n1 n2 ∗<br />

) ∧ ( f ) (ωFS) ∧ ...∧ ( f ns ∗<br />

) (ωFS) ∧ χω k−p+r−s<br />

FS .<br />

Using the case of (r − 1,s − 1) we can bound the first integral by cdn(r−1) .Stokes’<br />

theorem implies that the second integral is equal to<br />

�<br />

− T p−r ∧ ( f n2 ∗<br />

) (ωFS) ∧ ...∧ ( f ns ∗<br />

) (ωFS) ∧ (g ◦ f n1 c k−p+r−s<br />

)dd χ ∧ ωFS which is bounded by<br />

�g�∞�χ� C 2�T p−r ∧ ( f n2 ) ∗ (ωFS) ∧ ...∧ ( f ns ) ∗ (ωFS)�Wr,s−1<br />

since χ has support in Wr,s−1. We obtain the result using the (r,s − 1) case. ⊓⊔<br />

The above result suggests a local indicator of volume growth. Define for a ∈ P k<br />

lov( f ,a) := inf<br />

r>0 limsup<br />

1<br />

n<br />

n→∞<br />

logvolume(Π −1<br />

0 (Br) ∩Γn),<br />

where Br is the ball of center a and of radius r. We can show that if a ∈ Jp \ Jp+1<br />

and if Br does not intersect Jp+1, the above limsup is in fact a limit and is equal<br />

to plogd. One can also consider the graph of f n instead of Γn. The notion can be<br />

extended to meromorphic maps and its sub-level sets are analogues of Julia sets.<br />

We discuss now the metric entropy, i.e. the entropy of an invariant measure, a<br />

notion due to Kolgomorov-Sinai. Let g : X → X be map on a space X which is measurable<br />

with respect to a σ-algebra F .Letν be an invariant probability measure<br />

for g. Letξ = {ξ1,...,ξm} be a measurable partition of X. The entropy of ν with<br />

respect to ξ is a measurement of the information we gain when we know that a<br />

point x belongs to a member of the partition generated by g −i (ξ ) with 0 ≤ i ≤ n −1.<br />

The information we gain when we know that a point x belongs to ξi is a positive<br />

function I(x) which depends only on ν(ξi), i.e.I(x) =ϕ(ν(ξi)). The information<br />

given by independent events should be additive. In other words, we have<br />

ϕ(ν(ξi)ν(ξ j)) = ϕ(ν(ξi)) + ϕ(ν(ξ j))<br />

for i �= j. Hence, ϕ(t) =−clogt with c > 0. With the normalization c = 1, the<br />

information function for the partition ξ is defined by<br />

I ξ (x) := ∑−logν(ξi)1 ξi (x).

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