A Geometric Derivation of the Anomalous Magnetic Moment of the Electron in the Ω-Model

We present a geometric derivation of the anomalous magnetic moment of the electron within the framework of the Ω-model. In this model, time is treated as a complexvariable. Magnetism is derived from the compactified torsional curvature, leading to a vector potential. In the ideal (Dirac) case the electron’s g-factor is 2. However, when the compactified nature of time is taken into account, the torsional frequency acquires a small imaginary correction. We show that this complex correction yields a shift in the effective magnetic moment. A preliminary analysis indicates that the fractional shift is of order ∼ 2 × 10^−3, in good agreement with the experimental value of the electron anomaly. Our derivation is strictly geometric, relying only on the dual-frequency structure and compactified time, and requires no arbitrary scaling parameters.