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Discrete Holomorphic Local Dynamical Systems

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Dynamics of Rational Surface Automorphisms 83<br />

which would be exactly what you would obtain G + and G − were smooth and you<br />

integrate by parts: � χdd c G + ∧ dd c G − = � χdd c (G + ∧ μ − )= � (dd c χ) ∧ (G + ∧<br />

μ − ). This defines μ as a distribution. But since μ ± are a positive currents, we see<br />

that (*) defines μ as a positive distribution, and thus a measure.<br />

A variant of the convergence theorem above deals with the normalized pullbacks<br />

d −n f n∗ (χμ + )=χ( f n )μ + :<br />

Theorem 1.39. Let χ be a test function, and let c = � χμ.Then<br />

lim<br />

n→∞ d−n f ∗n (χμ + )= lim<br />

n→∞ χ( f n )μ + = cμ + .<br />

A measure ν is said to be mixing with respect to a transformation f if limn→∞ ν(A∩<br />

f −n B)=ν(A)ν(B) for all Borel sets A and B. For this, it suffices to show that for<br />

every pair of smooth functions ϕ and ψ,wehave<br />

�<br />

lim<br />

n→∞<br />

ϕ( f n �<br />

)ψμ=<br />

�<br />

ϕμ<br />

ψμ<br />

Corollary 1.40. The measure μ is mixing (and thus ergodic).<br />

Proof. We have � ϕ( f n )ψμ= � (ϕ( f n )μ + ) ∧ (ψμ − ),soasn → ∞, the right hand<br />

integral converges to � (cμ + ) ∧ ψμ − = c � ψμ + ∧ μ − = c � ψμ, and the constant is<br />

c = � ϕμ. ⊓⊔<br />

2 Rational Surfaces<br />

2.1 Blowing Up<br />

In the second section of these notes, we will consider automorphisms of a compact,<br />

rational surface M. Given an automorphism f ∈ Aut(M), we can look at its pullback<br />

on cohomology f ∗ ∈ GL(H 2 (M)). The dynamical degree is then defined as<br />

λ ( f ) := lim<br />

n→∞ || f n∗ || 1/n .<br />

A surface M ′ that is birationally equivalent to M may be topologically different:<br />

for instance, H 2 (M ′ ) and H 2 (M) can have different dimensions, and so the induced<br />

maps on cohomology will not be conjugate. However, in [DF]itisshownthatλ ( f )<br />

is the same for all birationally equivalent maps.<br />

Here we will focus on automorphisms for which λ ( f ) > 1. Although we will not<br />

discuss entropy here, we note that in this case the entropy is log(λ ( f )) > 0. Much of<br />

the theory for Hénon maps can be carried over to the case of automorphisms of compact<br />

surfaces. However, the Hénon family of diffeomorphisms themselves will not<br />

be part of this section: for a Hénon map H, there is no compact, complex manifold<br />

M which compactifies C 2 in such a way that H becomes a homeomorphism of M.

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