469 FCFG-D: A Dynamical Extension of Fractal-Continued-Fraction Geometry

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12   0  
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2026/09/27
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4 mins read
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FCFG-D: A Dynamical Extension of Fractal-Continued-Fraction Geometry


Author: Zhang Suhang (Luoyang, Henan)


Abstract


Within the FCFG framework, this paper unifies finite continued fractions, finite self-similar fractals, and the recursive structure of discrete dynamical systems. We define dynamical recursive systems and dynamical recursive invariants, propose the FCFG-D isomorphism axiom, prove the correspondence between rotation numbers, Lyapunov exponents, and continued-fraction coefficient sequences, and discuss the continued-fraction encoding of the KAM theorem, symbolic dynamics, and chaos.


Keywords: FCFG; dynamical recursion; continued fractions; rotation number; Lyapunov exponent; chaos


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1 Introduction


FCFG establishes an isomorphism between finite continued fractions and finite self-similar fractals:


r_n = S_n


This paper extends it to dynamics. The core observation:


Dynamics is iteration, iteration is recursion, recursion is the core of FCFG.


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2 Preliminaries


Finite continued fraction:


r_n = \cfrac{1}{a_1+\cfrac{1}{a_2+\cdots+\cfrac{1}{a_n}}}


FCFG isomorphism axiom:


r_n = S_n


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3 Dynamical Recursive Systems


Definition 3.1 Let X be a state space, f:X\to X. The n-th order iteration:


x_k = f^k(x_0)


Definition 3.2 If f can be decomposed as:


f = f_{a_1}\circ f_{a_2}\circ\cdots\circ f_{a_n}


this is called a dynamical recursive structure.


Definition 3.3 Let \lambda_n be a dynamical invariant. If it satisfies a recursion isomorphic to the continued-fraction recursion:


\lambda_k = \Phi(a_k,\lambda_{k-1})


then \lambda_n is called a dynamical recursive invariant.


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4 FCFG-D Isomorphism Axiom


Axiom 4.1 For any dynamical recursive system \mathcal{D}_n, there exist an arithmetic recursive system \mathcal{A}_n and a geometric recursive system \mathcal{G}_n such that:


\mathcal{A}_n \cong \mathcal{G}_n \cong \mathcal{D}_n


and


r_n = S_n = \lambda_n


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5 Rotation Number and Continued Fractions


Theorem 5.1 Let f:S^1\to S^1 be a circle map with rotation number \omega. Then the continued-fraction coefficients a_k of \omega correspond to the geometric recursive scaling sequence.


Proof: The rotation number is defined as:


\omega = \lim_{n\to\infty}\frac{F^n(x)-x}{n}


Its continued-fraction expansion is \omega=[a_1;a_2,\dots]. By Axiom 4.1, a_k is isomorphic to the geometric recursive scaling sequence. \square


Corollary 5.2


· \omega rational ⇔ periodic orbit ⇔ finite continued fraction

· \omega irrational ⇔ quasi-periodic orbit ⇔ infinite continued fraction

· \omega quadratic irrational ⇔ periodic continued fraction ⇔ self-similar geometric recursion


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6 Stability and Boundedness


Theorem 6.1 a_k bounded ⇔ dynamical system stable ⇔ geometric recursive dimension finite.


Proof: Boundedness of a_k corresponds to the Diophantine condition:


\left|\omega-\frac{p}{q}\right| > \frac{C}{q^{2+\epsilon}}


This is precisely the existence condition for KAM invariant tori. By Axiom 4.1, the geometric recursive dimension is determined by a_k, and boundedness implies finiteness. \square


Theorem 6.2 a_k unbounded ⇔ dynamical system chaotic ⇔ geometric recursive dimension divergent.


Proof: Unboundedness of a_k means slow continued-fraction approximation and unstable orbits. By Axiom 4.1, the geometric recursive dimension diverges. \square


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7 Lyapunov Exponent and Continued Fractions


Theorem 7.1 The Lyapunov exponent \lambda satisfies:


\lambda \sim \lim_{n\to\infty}\frac{1}{n}\log q_n


where q_n is the denominator of the n-th continued-fraction convergent.


Proof: q_n satisfies the recursion:


q_n = a_n q_{n-1} + q_{n-2}


The growth rate is determined by a_k. The Lyapunov exponent characterizes the rate of orbital separation and is isomorphic to q_n by Axiom 4.1. \square


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8 Symbolic Dynamics and Continued-Fraction Encoding


Theorem 8.1 Periodic orbits of chaotic systems can be encoded by continued-fraction coefficient sequences.


Proof: Symbolic dynamics maps orbits to symbol sequences. The continued-fraction coefficient sequence a_1,a_2,\dots itself constitutes a symbol sequence. By Axiom 4.1, dynamical recursion is isomorphic to arithmetic recursion, and periodic orbits correspond to periodic continued-fraction coefficients. \square


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9 Iterated Function Systems


The IFS is defined as:


F = \bigcup_{i=1}^{N}\phi_i(F)


where \phi_i are contraction mappings. The IFS is dynamics + geometric recursion. By Axiom 4.1, the contraction ratio sequence corresponds to the continued-fraction coefficient sequence.


The IFS is the geometric realization of FCFG-D.


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10 Discussion and Conclusion


Relationship with KAM: The existence of invariant tori is determined by the Diophantine condition on the rotation number, i.e., the boundedness of the continued-fraction coefficients.


Relationship with chaos: Periodic orbits, Lyapunov exponents, and attractor dimensions can all be encoded by continued fractions.


Limitations: Only applicable to finite-order, recursively decomposable dynamical systems; general dynamical systems do not necessarily satisfy Axiom 4.1.


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This paper establishes an isomorphism between dynamical recursion and arithmetic recursion, geometric recursion. The main results are:


1. Definition of dynamical recursive systems;

2. The FCFG-D isomorphism axiom;

3. The rotation number–continued fraction correspondence theorem;

4. The stability–boundedness correspondence theorems;

5. The Lyapunov exponent–continued fraction relation;

6. The symbolic dynamics continued-fraction encoding theorem;

7. The FCFG-D interpretation of IFS.


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References


[1] Original framework materials of FCFG.


[2] Continued fractions and Diophantine approximation.


[3] KAM theorem and rotation number theory.


[4] Chaos and symbolic dynamics.


[5] Iterated function systems and fractal geometry.


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