Quantized Topological Charge via Second Chern Number in SU(2) Gauge Theory — E8 Intelligence Research

FINDING: Non-Abelian gauge theory's topological charge is quantized via the second Chern number, with the integral of the Chern-Simons form yielding \(8\pi^2\) per instanton — a volume in SU(2) group space that encodes the winding of the gauge field. | MATH: The second Chern number for SU(2) is \(C_2 = \frac{1}{8\pi^2} \int \text{Tr}(F \wedge F)\), where \(F = dA + A \wedge A\). For a single instanton, \(\int \text{Tr}(F \wedge F) = 8\pi^2\), so \(C_2 = 1\). The non-Abelian Berry phase generalizes the Abelian case: \(\gamma = \mathcal{P} \exp(i \oint A_\mu dx^\mu)\), with \(A_\mu\) a matrix-valued connection. The volume of SU(2) is \(2\pi^2\) (the 3-sphere volume), and \(8\pi^2 = 4 \times 2\pi^2\) — a factor of 4 reflecting the quaternionic structure (SU(2) ≅ S³). | CONNECTION: The \(8\pi^2\) constant is deeply geometric: it equals \(4 \times (2\pi^2)\), where \(2\pi^2\) is the volume of the unit 3-sphere. This ties to the Hopf fibration \(S^1 \to S^3 \to S^2\) and the quaternion norm. 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
2026-09-29
DOI
https://doi.org/10.5281/zenodo.23030824
Primary Topic
Algebraic and Geometric Analysis
Type
preprint
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Quantized Topological Charge via Second Chern Number in SU(2) Gauge Theory — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Algebraic and Geometric Analysis
preprint

Quantized Topological Charge via Second Chern Number in SU(2) Gauge Theory — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Non-Abelian gauge theory's topological charge is quantized via the second Chern number, with the integral of the Chern-Simons form yielding \(8\pi^2\) per instanton — a volume in SU(2) group space that encodes the winding of the gauge field. | MATH: The second Chern number for SU(2) is \(C_2 = \frac{1}{8\pi^2} \int \text{Tr}(F \wedge F)\), where \(F = dA + A \wedge A\). For a single instanton, \(\int \text{Tr}(F \wedge F) = 8\pi^2\), so \(C_2 = 1\). The non-Abelian Berry phase generalizes the Abelian case: \(\gamma = \mathcal{P} \exp(i \oint A_\mu dx^\mu)\), with \(A_\mu\) a matrix-valued connection. The volume of SU(2) is \(2\pi^2\) (the 3-sphere volume), and \(8\pi^2 = 4 \times 2\pi^2\) — a factor of 4 reflecting the quaternionic structure (SU(2) ≅ S³). | CONNECTION: The \(8\pi^2\) constant is deeply geometric: it equals \(4 \times (2\pi^2)\), where \(2\pi^2\) is the volume of the unit 3-sphere. This ties to the Hopf fibration \(S^1 \to S^3 \to S^2\) and the quaternion norm. Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Algebraic and Geometric Analysis
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Quantized Topological Charge via Second Chern Number in SU(2) Gauge Theory — E8 Intelligence Research — Andrew Stewart Caldin · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS