Abstract
Let f(z) be entire i.e. analytic in the finite whole plane Z. The order of f(z) is defined aswhere A ray χ(θ) = {z = r·eiθ : 0 < r < + ∞} is called a Julia direction of f(z) if, in any open sector containing the ray, f(z) takes all values of Z, with at most one finite exceptional value, infinitely often.
Publisher
Cambridge University Press (CUP)