Abstract

Let Fq\mathbb{F}_q be the finite field of order qq, and P1(Fq)=Fq∪{∞}\mathbb P^1(\mathbb{F}_q) = \mathbb F_q\cup \{\infty\}. Write (x+y)m(x+\sqrt y)^m as N(x,y)+D(x,y)yN(x,y)+D(x,y)\sqrt{y}. For m∈Nm\in\mathbb N and a∈Fqa \in \mathbb{F}_q, the Rédei function Rm,a ⁣:P1(Fq)→P1(Fq)R_{m,a}\colon \mathbb P^1(\mathbb F_q) \to \mathbb P^1(\mathbb F_q) is defined by N(x,a)/D(x,a)N(x,a)/D(x,a) if D(x,a)≠0D(x,a)\neq 0 and x≠∞x\neq\infty, and ∞\infty, otherwise. In this paper we give a complete characterization of all pairs (m,n)∈N2(m,n)\in\mathbb N^2 such that the Rédei permutations Rm,aR_{m,a} and Rn,bR_{n,b} have the same cycle structure when aa and bb have the same quadratic character and qq is odd. We explore some relationships between such pairs (m,n)(m,n), and provide explicit families of Rédei permutations with the same cycle structure. When a Rédei permutation has a unique cycle structure that is not shared by any other Rédei permutation, we call it isolated. We show that the only isolated Rédei permutations are the isolated Rédei involutions. Moreover, all our results can be transferred to bijections of the form mxmx and xmx^m on certain domains.

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