Quaternion SO(3) Order Parameters Govern Icosahedral Selection in Liquid-to-Quasicrystal Transitions — E8 Intelligence Research

FINDING: Orientational order in liquid-to-quasicrystal transitions is governed by quaternion (SO(3)) order parameters whose symmetry-allowed invariants select icosahedral (Ih) rather than cubic or nematic phases. | MATH: Orientational order parameter Q_ij = ⟨n_i n_j − ⅓δ_ij⟩ (traceless symmetric, 5 independent components); quaternion q = (w, x, y, z), |q|² = 1, rotation R(q) ∈ SO(3) ≅ SU(2)/Z₂. Landau free energy F = a·Tr(Q²) + b·Tr(Q³) + c·(Tr(Q²))² + …; icosahedral invariant requires the cubic term Tr(Q³) to vanish by symmetry, forcing a **second-order** transition (unlike nematic, which is first-order). Icosahedral point group I_h order 120 = 2×60; rotational subgroup I order 60 ≅ A₅. | CONNECTION: Icosahedral symmetry is the maximal finite rotation group in 3D compatible with **five-fold axes** — the same 5-fold symmetry that generates φ = 1.618… via the icosahedron's vertex coordinates (±1, ±φ, 0) and cyclic permutations. The 6 five-fold axes of the icosahedron correspond to the 6 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
2026-10-30
DOI
https://doi.org/10.5281/zenodo.23796398
Primary Topic
Quasicrystal Structures and Properties
Type
preprint
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preprint

Quaternion SO(3) Order Parameters Govern Icosahedral Selection in Liquid-to-Quasicrystal Transitions — E8 Intelligence Research

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

Quaternion SO(3) Order Parameters Govern Icosahedral Selection in Liquid-to-Quasicrystal Transitions — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Orientational order in liquid-to-quasicrystal transitions is governed by quaternion (SO(3)) order parameters whose symmetry-allowed invariants select icosahedral (Ih) rather than cubic or nematic phases. | MATH: Orientational order parameter Q_ij = ⟨n_i n_j − ⅓δ_ij⟩ (traceless symmetric, 5 independent components); quaternion q = (w, x, y, z), |q|² = 1, rotation R(q) ∈ SO(3) ≅ SU(2)/Z₂. Landau free energy F = a·Tr(Q²) + b·Tr(Q³) + c·(Tr(Q²))² + …; icosahedral invariant requires the cubic term Tr(Q³) to vanish by symmetry, forcing a **second-order** transition (unlike nematic, which is first-order). Icosahedral point group I_h order 120 = 2×60; rotational subgroup I order 60 ≅ A₅. | CONNECTION: Icosahedral symmetry is the maximal finite rotation group in 3D compatible with **five-fold axes** — the same 5-fold symmetry that generates φ = 1.618… via the icosahedron's vertex coordinates (±1, ±φ, 0) and cyclic permutations. The 6 five-fold axes of the icosahedron correspond to the 6 Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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