Golden Oscillators: Fibonacci Spectra via Two-Base Quantum Calculus — E8 Intelligence Research

FINDING: Quantum calculus with two bases (Golden and Silver ratios) defines Fibonacci divisors and a Binet-form number operator, yielding a hierarchy of N=2 supersymmetric "Golden oscillators" with Fibonacci energy spectra. | MATH: Let \(q_1 = \phi = (1+\sqrt{5})/2\), \(q_2 = \Phi = (1-\sqrt{5})/2 = -1/\phi\). Fibonacci divisor derivative: \(\partial_{q_1,q_2} f(x) = [f(q_1 x) - f(q_2 x)]/[(q_1 - q_2)x]\). Binet number operator: \(\hat{N} = (\phi^n - \Phi^n)/\sqrt{5}\) acting on Fock states \(|n\rangle\). Energy spectrum: \(E_n \propto F_n = (\phi^n - \Phi^n)/\sqrt{5}\). Supersymmetric pair: bosonic \(a^\dagger a = F_{\hat{N}}\), fermionic \(b^\dagger b = F_{\hat{N}-1}\), with Witten index \(\text{Tr}(-1)^F = 0\) for finite hierarchy, but non-trivial for infinite hierarchy. | CONNECTION: The two bases are exactly \(\phi = 1.618...\) and \(\Phi = -0.618...\) — the positive and negative roots of \(x^2 - x - 1 = 0\). Their ratio \(\Phi/\phi = -0.382...\) (the negative of the golden ratio Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-04
DOI
https://doi.org/10.5281/zenodo.23131898
Primary Topic
Advanced Mathematical Theories and Applications
Type
preprint
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preprint

Golden Oscillators: Fibonacci Spectra via Two-Base Quantum Calculus — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Theories and Applications
preprint

Golden Oscillators: Fibonacci Spectra via Two-Base Quantum Calculus — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Quantum calculus with two bases (Golden and Silver ratios) defines Fibonacci divisors and a Binet-form number operator, yielding a hierarchy of N=2 supersymmetric "Golden oscillators" with Fibonacci energy spectra. | MATH: Let \(q_1 = \phi = (1+\sqrt{5})/2\), \(q_2 = \Phi = (1-\sqrt{5})/2 = -1/\phi\). Fibonacci divisor derivative: \(\partial_{q_1,q_2} f(x) = [f(q_1 x) - f(q_2 x)]/[(q_1 - q_2)x]\). Binet number operator: \(\hat{N} = (\phi^n - \Phi^n)/\sqrt{5}\) acting on Fock states \(|n\rangle\). Energy spectrum: \(E_n \propto F_n = (\phi^n - \Phi^n)/\sqrt{5}\). Supersymmetric pair: bosonic \(a^\dagger a = F_{\hat{N}}\), fermionic \(b^\dagger b = F_{\hat{N}-1}\), with Witten index \(\text{Tr}(-1)^F = 0\) for finite hierarchy, but non-trivial for infinite hierarchy. | CONNECTION: The two bases are exactly \(\phi = 1.618...\) and \(\Phi = -0.618...\) — the positive and negative roots of \(x^2 - x - 1 = 0\). Their ratio \(\Phi/\phi = -0.382...\) (the negative of the golden ratio Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Theories and Applications
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