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Periodic points and dynamic rays of exponential maps. (English) Zbl 1088.30017

The paper is concerned with the dynamics of the entire functions \(E_\lambda(z)=\lambda \exp z= \exp(z+\kappa)\) where \(\lambda=\exp\kappa\). Let \(S\) be the set of integer sequences \(s=s_1s_2s_3\dots\) and let \(\sigma:S\to S\) be the shift map: \(\sigma(s_1s_2s_3\dots)=s_2 s_3 s_4\dots\). A dynamic ray (or external ray) is an injective curve \(g_s:(0,\infty)\to {\mathbf C}\) satisfying \(\lim_{t\to\infty} \operatorname{Re} g_s(t) =\infty\), \(E_\lambda(g_s(t))=g_{\sigma(s)}(e^t-1)\), and \(g_s(t)=t-\kappa+2\pi i s_1+r_s(t)\), where \(r_s(t)< 2 e^{-t}(| \kappa| +C)\) for some constant \(C\). Such dynamic rays are known to exist for bounded (and in fact more general) sequences \(s\). A dynamic ray is said to land if \(\lim_{t\to 0} g_s(t)\) exists. The limit is then called a landing point.
The paper gives a thorough study of dynamic rays and their landing properties. In particular it is shown that periodic rays always land if the orbit of \(0\) is bounded. On the other hand, it is shown that in many dynamically important cases every repelling or parabolic periodic point is a landing point of a periodic dynamic ray. It is also shown that if \(0\) is preperiodic, then \(0\) is the landing point of at least one preperiodic dynamic ray.
Note: Using results by D. Schleicher on the parameter space of exponentials, L. Rempe has recently shown that periodic dynamic rays always land.

MSC:

30D05 Functional equations in the complex plane, iteration and composition of analytic functions of one complex variable
33B10 Exponential and trigonometric functions
37B10 Symbolic dynamics
37C25 Fixed points and periodic points of dynamical systems; fixed-point index theory; local dynamics
37F10 Dynamics of complex polynomials, rational maps, entire and meromorphic functions; Fatou and Julia sets
37F20 Combinatorics and topology in relation with holomorphic dynamical systems