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Discrete Holomorphic Local Dynamical Systems

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Dynamics of Rational Surface Automorphisms 89<br />

Corollary 2.9. If η is an eigenvalue of f ∗ , then either η = λ ,λ −1 ,or|η| = 1.<br />

Proof. We have seen that λ ( f ) is the only eigenvalue of modulus > 1. Now we know<br />

that ( f ∗ ) −1 =(f −1 ) ∗ ,soifη is an eigenvalue of f ∗ ,thenη −1 is an eigenvalue of<br />

( f −1 ) ∗ . Applying the Theorem to f −1 , we conclude that λ is the only eigenvalue<br />

for ( f −1 ) ∗ which is > 1. ⊓⊔<br />

Let χ f denote the characteristic polynomial of f ∗ . It follows that χ f is monic, and<br />

the constant term (the determinant of f ∗ , an invertible matrix) is ±1. Let ψ f denote<br />

the minimal polynomial of λ . By the Theorem, we see that except for λ and 1/λ ,<br />

all zeros of χ f (and thus all zeros of ψ f ) lie on the unit circle. Such a polynomial ψ f<br />

is called a Salem polynomial,andλ is a Salem number. We may factor χ f = C · ψ f ,<br />

where C is a polynomial whose coefficients belong to Z, and the roots of C lie in the<br />

unit circle. It follows by elementary number theory that the zeros of C are roots of<br />

unity.<br />

The following is a heuristic argument for the existence of a positive, closed invariant<br />

1,1-current. Suppose that X is a Kähler surface and that f ∈ Aut(X) has<br />

λ ( f ) > 1. Let ω + be a positive, smooth cohomology class which is an eigenvector<br />

of λ . By this we mean that there is a smooth form ω + such that the cohomology<br />

class is expanded<br />

{ f ∗ ω + } = f ∗ {ω + } = λ {ω + }.<br />

Thus f ∗ ω + − λω + is cohomologous to zero, and thus there is a smooth function γ +<br />

such that<br />

1<br />

λ f ∗ ω + − ω + = dd c γ + .<br />

If we can take ω + to be poisitive, then f ∗ ω + will be positive, and we see that γ +<br />

is essentially pluri-subharmonic, i.e., dd c γ + + ω + ≥ 0. Applying λ −1 f ∗ repeatedly,<br />

we find<br />

If we define<br />

1<br />

λ 2 f ∗2 ω + − 1<br />

λ f ∗ ω + = 1<br />

λ ddc f ∗ γ + = 1<br />

λ ddcγ + ◦ f<br />

1<br />

λ n f ∗n ω + − 1<br />

λ n−1 f ∗(n−1) ω + = 1<br />

λ n−1 ddcγ + ◦ f n−1 .<br />

g + =<br />

∞ γ<br />

∑<br />

n=0<br />

+ ◦ f n<br />

λ n , T + = ω + + dd c g + ,<br />

then we see that g + is continuous, since the defining series converges uniformly.<br />

Further, T + is a positive, closed current with the invariance property f ∗ T + = λ T + .<br />

We may apply the same argument with f −1 and the eigenvalue λ −1 obtain a positive,<br />

closed current T − with the property that ( f −1 ) ∗ T − = λ T − . We may obtain an<br />

invariant measure μ := T + ∧ T − .<br />

Notes The currents T ± and measure μ have been shown to have many of the same<br />

properties that were found for the Hénon family (see [C2,Du]). Much of this theory<br />

may be carried over to more general meromorphic surface mappings; one recent<br />

work in this direction is [DDG1–3].

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