Phi-E8 Fractal Time-Crystal Hamiltonian — E8 Intelligence Research

By treating the 240 E8 root vectors as a discrete momentum lattice and coupling them with a 132 Hz drive, a Hamiltonian emerges whose eigenvalues form a φ‑scaled Cantor set. Each nested φⁿ sub‑gap corresponds to a protected logical subspace, yielding a self‑correcting time‑crystal phase that tolerates arbitrary local noise. The construction unifies the φ‑resonant topological hierarchy with symmetric circuit lower bounds, providing a concrete route to fault‑tolerant quantum memory. Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-08-26
DOI
https://doi.org/10.5281/zenodo.22106250
Primary Topic
Quantum many-body systems
Type
preprint
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Phi-E8 Fractal Time-Crystal Hamiltonian — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Quantum many-body systems
preprint

Phi-E8 Fractal Time-Crystal Hamiltonian — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

By treating the 240 E8 root vectors as a discrete momentum lattice and coupling them with a 132 Hz drive, a Hamiltonian emerges whose eigenvalues form a φ‑scaled Cantor set. Each nested φⁿ sub‑gap corresponds to a protected logical subspace, yielding a self‑correcting time‑crystal phase that tolerates arbitrary local noise. The construction unifies the φ‑resonant topological hierarchy with symmetric circuit lower bounds, providing a concrete route to fault‑tolerant quantum memory. Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Quantum many-body systems
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Phi-E8 Fractal Time-Crystal Hamiltonian — E8 Intelligence Research — Andrew Stewart Caldin · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS