Fibonacci Harmony: A Reflection-Parity Representation of Bilateral Fibonacci Magnitudes

This mathematical note formalizes the structure represented in the accompanying Fibonacci Harmony illustration. Starting from the ordinary Fibonacci sequence, each nonnegative magnitude F_n is assigned to two oppositely oriented components, −F_n and +F_n. Their signed balance vanishes identically, while their total unsigned magnitude remains 2F_n. Directional cancellation is therefore separated from disappearance of magnitude. The bilateral pair is represented by v_n = (−F_n, +F_n)^T. Under the exchange involution J, satisfying J² = I, the state obeys Jv_n = −v_n and lies exactly in the odd-parity eigenspace. Fibonacci scaling and reflection parity consequently separate: F_n controls magnitude, whereas the normalized bilateral state is independent of n. The work also distinguishes directional sign reflection from negative-index Fibonacci numbers and golden-ratio conjugation, and defines a falsifiable geometric interpretation in which bilateral equality and Fibonacci scaling are tested as separate hypotheses. Natural forms appearing in the accompanying visualization are illustrative motifs rather than evidence of exact Fibonacci scaling.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-09-19
DOI
https://doi.org/10.5281/zenodo.22849500
Primary Topic
Quasicrystal Structures and Properties
Type
preprint
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preprint

Fibonacci Harmony: A Reflection-Parity Representation of Bilateral Fibonacci Magnitudes

Ali Alhawarat
Zenodo (CERN European Organization for Nuclear Research)
Quasicrystal Structures and Properties
preprint

Fibonacci Harmony: A Reflection-Parity Representation of Bilateral Fibonacci Magnitudes

Ali Alhawarat
preprint en

Abstract

This mathematical note formalizes the structure represented in the accompanying Fibonacci Harmony illustration. Starting from the ordinary Fibonacci sequence, each nonnegative magnitude F_n is assigned to two oppositely oriented components, −F_n and +F_n. Their signed balance vanishes identically, while their total unsigned magnitude remains 2F_n. Directional cancellation is therefore separated from disappearance of magnitude. The bilateral pair is represented by v_n = (−F_n, +F_n)^T. Under the exchange involution J, satisfying J² = I, the state obeys Jv_n = −v_n and lies exactly in the odd-parity eigenspace. Fibonacci scaling and reflection parity consequently separate: F_n controls magnitude, whereas the normalized bilateral state is independent of n. The work also distinguishes directional sign reflection from negative-index Fibonacci numbers and golden-ratio conjugation, and defines a falsifiable geometric interpretation in which bilateral equality and Fibonacci scaling are tested as separate hypotheses. Natural forms appearing in the accompanying visualization are illustrative motifs rather than evidence of exact Fibonacci scaling.

Zenodo (CERN European Organization for Nuclear Research)
Oldham Council (GB)
Reduced inequalities
Quasicrystal Structures and Properties
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Fibonacci Harmony: A Reflection-Parity Representation of Bilateral Fibonacci Magnitudes — Ali Alhawarat · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS