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Rédei Functions: Conics and Cryptography

Updated 8 July 2026
  • Rédei functions are rational functions defined by decomposing (z+√d)ⁿ into polynomial parts, encapsulating group laws on Pell conics and their generalizations.
  • They are characterized by explicit power formulas, recurrence relations, and matrix representations that unify quadratic algebra with conic geometry.
  • Rédei functions underpin practical applications in cryptography and rational approximation, serving as the computational core in RSA-like schemes and polynomial Pell equations.

Searching arXiv for recent and foundational papers on Rédei functions and closely related finite-field, conic, Pell, and classification contexts. Rédei functions are rational functions arising from powers in quadratic extensions and from group laws on conics, with classical roots in Pell-type arithmetic and modern manifestations in finite-field permutation theory, cryptography, and exceptional rational function classification. In the classical setting, they are defined from the expansion

(z+d)n=Nn(d,z)+Dn(d,z)d,(z+\sqrt d)^n = N_n(d,z)+D_n(d,z)\sqrt d,

with the associated rational function

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},

while a broader two-parameter generalization replaces the quadratic relation x2=dx^2=d by x2hxd=0x^2-hx-d=0 and yields

Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.

These functions encode repeated composition under explicit algebraic group laws, especially on Pell-type conics, and over finite fields they also appear as permutation rational functions on P1(Fq)\mathbb P^1(\mathbb F_q), often called Rédei permutations (Barbero et al., 2011, Barbero et al., 2012).

1. Classical definition and algebraic origin

Classically, Rédei functions are built from the decomposition of (z+d)n(z+\sqrt d)^n into its d\sqrt d-free and d\sqrt d-linear parts: (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d}, where

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},0

The associated Rédei rational function is

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},1

This construction is the basic one in Pell theory and is also the specialization Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},2 of the generalized family studied later on conics (Barbero et al., 2011, Barbero et al., 2012).

A matrix realization makes the structure transparent. In the classical case,

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},3

which immediately yields the addition formulas

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},4

In the generalized setting one replaces this matrix by

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},5

and defines

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},6

When Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},7, this recovers the usual Rédei rational functions exactly (Barbero et al., 2012).

The algebraic source is the quadratic algebra

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},8

with multiplication induced by Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},9. In this framework, powers of x2=dx^2=d0 generate the polynomial sequences x2=dx^2=d1 and x2=dx^2=d2, and the quotient x2=dx^2=d3 encodes the corresponding power in rational form. This mechanism underlies both the classical Pell interpretation and the generalized conic theory (Barbero et al., 2012).

Both the classical and generalized polynomial sequences satisfy second-order linear recurrences. In the classical case,

x2=dx^2=d4

equivalently

x2=dx^2=d5

x2=dx^2=d6

In the generalized case both satisfy

x2=dx^2=d7

with initial data

x2=dx^2=d8

These recurrence structures are central in both theoretical manipulations and efficient computation (Barbero et al., 2011, Barbero et al., 2012).

2. Conics, Pell geometry, and group laws

The most direct structural interpretation of Rédei functions is via conic group laws. In the generalized setting, the relevant conic is

x2=dx^2=d9

Under the identification x2hxd=0x^2-hx-d=00 in the quadratic algebra x2hxd=0x^2-hx-d=01, the norm

x2hxd=0x^2-hx-d=02

shows that the unit norm elements correspond exactly to the points of this conic (Barbero et al., 2012).

The induced product on the conic is

x2hxd=0x^2-hx-d=03

The paper states that x2hxd=0x^2-hx-d=04 is an abelian group with identity x2hxd=0x^2-hx-d=05 and inverse

x2hxd=0x^2-hx-d=06

When x2hxd=0x^2-hx-d=07, this becomes the Pell hyperbola

x2hxd=0x^2-hx-d=08

with group law

x2hxd=0x^2-hx-d=09

which is exactly the multiplication law inherited from Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.0 (Barbero et al., 2012).

A rational parametrization transports this conic group to a one-dimensional parameter set. With

Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.1

the parametrization map is

Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.2

and the inverse is

Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.3

for Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.4, together with

Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.5

Transporting the conic law to Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.6 gives

Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.7

with Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.8 when Qn(h,d,z)=Nn(h,d,z)Dn(h,d,z).Q_n(h,d,z)=\frac{N_n(h,d,z)}{D_n(h,d,z)}.9. The identity is P1(Fq)\mathbb P^1(\mathbb F_q)0. The generalized Rédei functions are precisely the powers in this parameter group (Barbero et al., 2012).

In the Pell case this reduction is especially explicit. On the extended line P1(Fq)\mathbb P^1(\mathbb F_q)1, the transported product is

P1(Fq)\mathbb P^1(\mathbb F_q)2

with identity P1(Fq)\mathbb P^1(\mathbb F_q)3, inverse P1(Fq)\mathbb P^1(\mathbb F_q)4, and an isomorphism from P1(Fq)\mathbb P^1(\mathbb F_q)5 given by

P1(Fq)\mathbb P^1(\mathbb F_q)6

Within this interpretation, Rédei functions are exactly the iterated powers: P1(Fq)\mathbb P^1(\mathbb F_q)7 This turns the addition law

P1(Fq)\mathbb P^1(\mathbb F_q)8

into the ordinary power law of the group P1(Fq)\mathbb P^1(\mathbb F_q)9 (Barbero et al., 2011).

A determinant identity ties these constructions back to the conic. Since

(z+d)n(z+\sqrt d)^n0

one gets

(z+d)n(z+\sqrt d)^n1

Hence, when

(z+d)n(z+\sqrt d)^n2

the pair (z+d)n(z+\sqrt d)^n3 lies on the conic (z+d)n(z+\sqrt d)^n4. This exhibits the polynomial pair itself as a generator of conic powers and thereby links recurrence, conic geometry, and rational parametrization in a single formalism (Barbero et al., 2012).

3. Composition, powers, and approximation theory

A fundamental property of classical Rédei functions is the multiplicative index law

(z+d)n(z+\sqrt d)^n5

which implies that Rédei functions commute under composition. In the group-law interpretation this is immediate: once (z+d)n(z+\sqrt d)^n6 is viewed as the (z+d)n(z+\sqrt d)^n7-th power of (z+d)n(z+\sqrt d)^n8 in the (z+d)n(z+\sqrt d)^n9-group, composition corresponds to multiplication of exponents (Barbero et al., 2011).

The generalized functions satisfy the analogous role on the parameter group of the conic. The paper on generalized Rédei functions emphasizes that they “play exactly the same structural role as in the Pell hyperbola”: they encode repeated composition under the group law and provide explicit formulas for powers of points over the conic (Barbero et al., 2012).

The same formalism also yields rational approximations to quadratic irrationalities. In the Pell setting, the paper explicitly emphasizes that d\sqrt d0 converges to d\sqrt d1, describing Rédei functions as “rational approximations of d\sqrt d2, for any parameter d\sqrt d3” (Barbero et al., 2011). The generalized conic paper extends this approximation viewpoint and states that it obtains “a new result for the approximation of quadratic irrationalities” (Barbero et al., 2012).

A polynomial analogue appears in the study of the polynomial Pell equation

d\sqrt d4

Using Rédei polynomials

d\sqrt d5

the identity

d\sqrt d6

produces explicit polynomial solutions once one chooses d\sqrt d7 and d\sqrt d8, so that d\sqrt d9. This yields all integer polynomial solutions for

d\sqrt d0

in the cases d\sqrt d1 described in the paper (Murru, 2019).

This suggests a unifying interpretation: Rédei functions and polynomials are compression devices for powers in quadratic algebras. In arithmetic settings, the compression is rational and suited to Pell-type groups; in polynomial settings, the same binomial decomposition yields complete families of Pell-type solutions (Barbero et al., 2011, Murru, 2019).

4. Finite-field Rédei functions and Rédei permutations

Over finite fields, Rédei functions become rational self-maps of the projective line

d\sqrt d2

For d\sqrt d3, writing

d\sqrt d4

one defines

d\sqrt d5

A Rédei function that induces a bijection on d\sqrt d6 is called a Rédei permutation (Capaverde et al., 2020, Capaverde et al., 2021).

A standard criterion is

d\sqrt d7

where d\sqrt d8 is the quadratic character. Since d\sqrt d9 is even for odd (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},0, no even (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},1 yields a Rédei permutation (Capaverde et al., 2020, Capaverde et al., 2021).

The cycle structure is controlled entirely by arithmetic modulo divisors of (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},2. If (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},3 is a permutation, then it consists of

(z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},4

disjoint (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},5-cycles for each divisor (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},6, together with (z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},7 fixed points. The total number of fixed points is

(z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},8

Moreover,

(z+d)n=Nn(d,z)+Dn(d,z)d,(z + \sqrt{d})^n = N_n(d, z) + D_n(d, z)\sqrt{d},9

These formulas place the dynamics of Rédei permutations squarely in the arithmetic of multiplicative orders (Capaverde et al., 2020).

A complete characterization of when two Rédei permutations have the same cycle structure is given in terms of the condition

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},00

assuming the parameters have the same quadratic character. The classification is then refined prime by prime using multiplicative orders and Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},01-adic valuation constraints (Capaverde et al., 2021).

Special attention has been given to Rédei permutations whose nontrivial cycles all have the same length. For cycle decompositions consisting only of Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},02-cycles and Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},03-cycles, with Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},04 prime, the paper gives an exact admissibility criterion for divisors Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},05 and an existence theorem: such a Rédei permutation exists if and only if Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},06 or Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},07 has a prime factor of the form Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},08 or is divisible by Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},09 (Capaverde et al., 2020).

A different finite-field presentation, especially useful structurally, expresses Rédei functions by Möbius conjugation. For odd Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},10, if Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},11 is irreducible over Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},12 and Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},13 is a root, define

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},14

Then Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},15 maps Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},16 bijectively onto Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},17, the group of Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},18-st roots of unity in Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},19. As a result, the functional graph of Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},20 on Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},21 is isomorphic to that of Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},22 on Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},23, and

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},24

in that nonsquare setting (Ding et al., 2021).

This Möbius-conjugation viewpoint also yields an addition law: Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},25 For odd Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},26, where Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},27, this simplifies to

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},28

This is the finite-field counterpart of the Pell-style addition law seen over Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},29 (Ding et al., 2021).

5. Cryptographic and algorithmic roles

Rédei functions have been used as the computational core of RSA-like schemes based on conics, especially the Pell hyperbola. The central idea is to replace ordinary exponentiation by powering in a non-standard parameter group

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},30

or, in the generalized conic setting,

Qn(d,z)=Nn(d,z)Dn(d,z),Q_n(d,z)=\frac{N_n(d,z)}{D_n(d,z)},31

Since [ z{\

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