Abstract

Continuous generalizations of the Fibonacci sequence satisfy ODEs that are formal analogues of the Friedmann equation describing a spatially homogeneous and isotropic cosmology in general relativity. These analogies are presented together with their Lagrangian and Hamiltonian formulations and with an invariant of the Fibonacci sequence.

Highlights

  • Fibonacci, known as Leonardo Pisano or Leonardo Bonacci, introduced Hindu–Arabic numerals to Europe with his book Liber Abaci in 1202 [1]

  • We focus on F(e,o) ( x ), which admit analogies with relativistic cosmology, while no such analogy exists for F ( x )

  • Of which F(e) and F(o) are two linearly independent solutions. This equation describes the one-dimensional motion of a particle of position F in the inverted harmonic oscillator potential V ( F ) = −kF2 /2, which is used as an example of an unstable mechanical system

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Summary

Introduction

Arabic numerals to Europe with his book Liber Abaci in 1202 [1]. He posed and solved a well-known problem involving the growth of a population of rabbits in idealized situations. The ratio of two consecutive terms Fn+1 /Fn approaches the golden ratio. Reproduces part of the Fibonacci numbers, Fn = F(e) (n), for even x = n ∈ N, while. Reproduces the other Fibonacci numbers for odd x = n ∈ N. Of which F(e) and F(o) are two linearly independent solutions In physics, this equation describes the one-dimensional motion of a particle of position F in the inverted harmonic oscillator potential V ( F ) = −kF2 /2 (with K = 2 ln φ), which is used as an example of an unstable mechanical system (this property corresponds to the fact that the Fibonacci numbers Fn increase without bound as n → ∞). We briefly recall the basics of spatially homogeneous and isotropic cosmology in general relativity, and we present the formal analogy with.

FLRW Cosmology
The Cosmological Analogy
Lagrangian and Hamiltonian
Conclusions
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