Symmetry Breakdown in Posner Molecules Invalidates Quantum Spin Protection Model — E8 Intelligence Research

FINDING: The Posner molecule (Ca₉(PO₄)₆) — previously proposed as a biological quantum information processor via long-lived nuclear spins — is shown to lack the high symmetry (C₁ or C₃) assumed for its nuclear spin Hilbert space; its dynamical ensemble is not symmetric, invalidating the simple permutation-symmetry protection model. MATH: - Molecular point group: Ca₉(PO₄)₆ — actual symmetry is **C₁** (no nontrivial rotational or reflection symmetries) in the dynamical ensemble, not the idealized **C₃** or higher. - Nuclear spin Hilbert space dimension: For ⁴³Ca (I=7/2) and ³¹P (I=1/2), with 9 Ca and 6 P nuclei: dim(H) = (2·7/2+1)⁹ × (2·1/2+1)⁶ = 8⁹ × 2⁶ = 2²⁷ × 2⁶ = 2³³ ≈ 8.59×10⁹. - Symmetry reduction: Under C₃, the Hilbert space decomposes into irreducible representations (A, E) — but with C₁, no such block diagonalization; all 2³³ states mix under the molecular Hamiltonian. - Key result (arXiv:2108.08822v2): The dynamical ensemble average over molecular orientations and 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
2026-10-05
DOI
https://doi.org/10.5281/zenodo.23152244
Primary Topic
Quantum Mechanics and Applications
Type
preprint
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
preprint

Symmetry Breakdown in Posner Molecules Invalidates Quantum Spin Protection Model — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Quantum Mechanics and Applications
preprint

Symmetry Breakdown in Posner Molecules Invalidates Quantum Spin Protection Model — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: The Posner molecule (Ca₉(PO₄)₆) — previously proposed as a biological quantum information processor via long-lived nuclear spins — is shown to lack the high symmetry (C₁ or C₃) assumed for its nuclear spin Hilbert space; its dynamical ensemble is not symmetric, invalidating the simple permutation-symmetry protection model. MATH: - Molecular point group: Ca₉(PO₄)₆ — actual symmetry is **C₁** (no nontrivial rotational or reflection symmetries) in the dynamical ensemble, not the idealized **C₃** or higher. - Nuclear spin Hilbert space dimension: For ⁴³Ca (I=7/2) and ³¹P (I=1/2), with 9 Ca and 6 P nuclei: dim(H) = (2·7/2+1)⁹ × (2·1/2+1)⁶ = 8⁹ × 2⁶ = 2²⁷ × 2⁶ = 2³³ ≈ 8.59×10⁹. - Symmetry reduction: Under C₃, the Hilbert space decomposes into irreducible representations (A, E) — but with C₁, no such block diagonalization; all 2³³ states mix under the molecular Hamiltonian. - Key result (arXiv:2108.08822v2): The dynamical ensemble average over molecular orientations and 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 Mechanics and Applications
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.