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Discrete Holomorphic Local Dynamical Systems

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Dynamics in Several Complex variables 231<br />

Consider a more abstract setting. Let g : X → X be a measurable map and ν<br />

an invariant probability measure. Let A : X → GL(R,k) be a measurable function.<br />

Define for n ≥ 0<br />

An(x) := A(g n−1 (x))...A(x).<br />

These functions satisfy the identity<br />

An+m(x)=An(g m (x))Am(x)<br />

for n,m ≥ 0. We say that the sequence (An) is the multiplicative cocycle over X<br />

generated by A.<br />

The following Oseledec’s multiplicative ergodic theorem is related to the<br />

Kingman’s sub-multiplicative ergodic theorem [KH, W]. It can be seen as a generalization<br />

of the above property of a single square matrix A.<br />

Theorem 1.119 (Oseledec). Let g : X → X,ν and the cocycle (An) be as above. Assume<br />

that ν is ergodic and that log + �A ±1 (x)� are in L 1 (ν). Then there is an integer<br />

m, real numbers χ1 < ··· < χm, and for ν-almost every x, a unique decomposition<br />

of R k into a direct sum of linear subspaces<br />

such that<br />

R k m�<br />

= Ei(x)<br />

i=1<br />

1. The dimension of Ei(x) does not depend on x.<br />

2. The decomposition is invariant, that is, A(x) sends Ei(x) to Ei(g(x)).<br />

3. We have locally uniformly on vectors v in Ei(x) \{0}<br />

1<br />

lim<br />

n→∞ n log�An(x) · v� = χi.<br />

4. For S ⊂{1,...,m}, define ES(x) := ⊕i∈SEi(x).IfS,S ′ are disjoint, then the angle<br />

between ES(x) and E S ′(x) is a tempered function, that is,<br />

1<br />

lim<br />

n→∞ n logsin� �<br />

�∠ ES(g n (x)),ES ′(g n (x)) �� � = 0.<br />

The result is still valid for non-ergodic systems but the constants m and χi should<br />

be replaced with invariant functions. If g is invertible, the previous decomposition<br />

is the same for g −1 where the exponents χi are replaced with −χi. The result is also<br />

valid in the complex setting where we replace R with C and GL(R,k) by GL(C,k).<br />

In this case, the subspaces Ei(x) are complex.<br />

We now come back to a smooth dynamical system g : X → X on a compact<br />

manifold. We assume that the Jacobian J(g) of g associated to a smooth volume<br />

form satisfies 〈ν,logJ(g)〉 > −∞. Under this hypothesis, we can apply Oseledec’s<br />

theorem to the cocycle induced by g on the tangent bundle of X; this allows to<br />

decompose, ν-almost everywhere, the tangent bundle into invariant sub-bundles.

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