Chern Number Quantization of Hall Conductance via Berry Curvature on the Brillouin Zone Torus — E8 Intelligence Research

FINDING: Chern number is an integer-valued characteristic class in H²(T²,ℤ) that quantizes Hall conductance via the Berry curvature integral over the Brillouin zone torus. | MATH: c₁ = (1/2π) ∮_BZ F d²k ∈ ℤ; σ_xy = (e²/h) · c₁; F = ∂_kx A_ky − ∂_ky A_kx; A = i⟨u_k|∇_k|u_k⟩; TKNN formula: σ_xy = (e²/h)(1/2π)∫_BZ Ω(k) d²k. Half-BHZ model: c₁ = ±1/2 per band, ±1 total. Second Chern number: c₂ = (1/8π²)∫ Tr(F∧F) ∈ ℤ for 4D systems (4D QHE). | CONNECTION: The Brillouin zone is a 2-torus T² with lattice symmetry — the reciprocal lattice inherits crystallographic point group symmetries. Chern number quantization arises from the periodicity of the fiber bundle U(1) → total space → T². The integer quantization is topological, not geometric, but the underlying lattice (hexagonal for BHZ, square for Qi-Wu-Zhang) determines which Chern numbers are realizable. No direct golden ratio or Fibonacci connection in the Chern number itself. However: the Berry curvature distribution over the BZ respects th 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
2026-11-03
DOI
https://doi.org/10.5281/zenodo.23910070
Primary Topic
Topological Materials and Phenomena
Type
preprint
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Chern Number Quantization of Hall Conductance via Berry Curvature on the Brillouin Zone Torus — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Topological Materials and Phenomena
preprint

Chern Number Quantization of Hall Conductance via Berry Curvature on the Brillouin Zone Torus — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Chern number is an integer-valued characteristic class in H²(T²,ℤ) that quantizes Hall conductance via the Berry curvature integral over the Brillouin zone torus. | MATH: c₁ = (1/2π) ∮_BZ F d²k ∈ ℤ; σ_xy = (e²/h) · c₁; F = ∂_kx A_ky − ∂_ky A_kx; A = i⟨u_k|∇_k|u_k⟩; TKNN formula: σ_xy = (e²/h)(1/2π)∫_BZ Ω(k) d²k. Half-BHZ model: c₁ = ±1/2 per band, ±1 total. Second Chern number: c₂ = (1/8π²)∫ Tr(F∧F) ∈ ℤ for 4D systems (4D QHE). | CONNECTION: The Brillouin zone is a 2-torus T² with lattice symmetry — the reciprocal lattice inherits crystallographic point group symmetries. Chern number quantization arises from the periodicity of the fiber bundle U(1) → total space → T². The integer quantization is topological, not geometric, but the underlying lattice (hexagonal for BHZ, square for Qi-Wu-Zhang) determines which Chern numbers are realizable. No direct golden ratio or Fibonacci connection in the Chern number itself. However: the Berry curvature distribution over the BZ respects th Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Topological Materials and Phenomena
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