Rogers-Ramanujan Identities Link Affine Algebras to Quasicrystal 5-Fold Symmetry — E8 Intelligence Research

FINDING: Rogers-Ramanujan identities extend to affine Kac-Moody algebra \(A_{2n}^{(2)}\) families, directly linking to quasicrystal diffraction patterns with forbidden 5-fold symmetry. MATH: - Rogers-Ramanujan identities: \(\prod_{k=0}^{\infty} \frac{1}{(1-q^{5k+1})(1-q^{5k+4})} = \sum_{n=0}^{\infty} \frac{q^{n^2}}{(q;q)_n}\) \(\prod_{k=0}^{\infty} \frac{1}{(1-q^{5k+2})(1-q^{5k+3})} = \sum_{n=0}^{\infty} \frac{q^{n^2+n}}{(q;q)_n}\) - Generalised to \(A_{2n}^{(2)}\) at level \(m\): product side corresponds to specialised characters of this affine Lie algebra. - Quasicrystal diffraction patterns exhibit 5-fold rotational symmetry, forbidden in periodic crystals, with Fourier peaks at positions governed by golden ratio \(\phi = (1+\sqrt{5})/2 \approx 1.618\). - Penrose tiling inflation factor = \(\phi^2 = 2.618\), and deflation ratio = \(1/\phi \approx 0.618\). CONNECTION: - Golden ratio \(\phi\) appears directly: 5-fold symmetry in quasicrystals yields diffraction spo 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
2026-07-27
DOI
https://doi.org/10.5281/zenodo.21617496
Primary Topic
Quasicrystal Structures and Properties
Type
preprint
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Rogers-Ramanujan Identities Link Affine Algebras to Quasicrystal 5-Fold Symmetry — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Quasicrystal Structures and Properties
preprint

Rogers-Ramanujan Identities Link Affine Algebras to Quasicrystal 5-Fold Symmetry — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Rogers-Ramanujan identities extend to affine Kac-Moody algebra \(A_{2n}^{(2)}\) families, directly linking to quasicrystal diffraction patterns with forbidden 5-fold symmetry. MATH: - Rogers-Ramanujan identities: \(\prod_{k=0}^{\infty} \frac{1}{(1-q^{5k+1})(1-q^{5k+4})} = \sum_{n=0}^{\infty} \frac{q^{n^2}}{(q;q)_n}\) \(\prod_{k=0}^{\infty} \frac{1}{(1-q^{5k+2})(1-q^{5k+3})} = \sum_{n=0}^{\infty} \frac{q^{n^2+n}}{(q;q)_n}\) - Generalised to \(A_{2n}^{(2)}\) at level \(m\): product side corresponds to specialised characters of this affine Lie algebra. - Quasicrystal diffraction patterns exhibit 5-fold rotational symmetry, forbidden in periodic crystals, with Fourier peaks at positions governed by golden ratio \(\phi = (1+\sqrt{5})/2 \approx 1.618\). - Penrose tiling inflation factor = \(\phi^2 = 2.618\), and deflation ratio = \(1/\phi \approx 0.618\). CONNECTION: - Golden ratio \(\phi\) appears directly: 5-fold symmetry in quasicrystals yields diffraction spo Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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