Cyclic Phenomena for Composition Operators
Let H(U) be the set of all holomorphic functions on the unit ball U of the complex plane. The Hardy space H2 is the set of all functions f(z)= that belongs to H(U) such that < ¥. Let j be a holomorphic self map of U. The composition operator Cj on H2 is defined as follows:
Cjf = foj, for all f Î H2