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Dual magnetic and electric dipole symmetry: Pseudoangular momentum in parity space and the electric Landé g factor

Michael E. Tobar*

  • *Contact author: michael.tobar@uwa.edu.au

APS Open Sci. 1, 000057 – Published 7 July, 2026

DOI: https://doi.org/10.1103/xhk9-qt61

Abstract

Electric dipole moments (EDMs) are sensitive probes of fundamental symmetries and central to searches for physics beyond the standard model. We present a symmetry-based, Zeeman-analog operator framework that places magnetic and electric dipole physics on parallel footing under electromagnetic duality and introduce a polar-sector pseudo-angular-momentum degree of freedom in parity space together with an associated electric Landé g factor, gE, that organizes induced orbital dipoles. Following Ohanian's effective-current formulation of the Zeeman effect, we construct its electric dual: The wavefunction's microscopic polarization admits an equivalent effective magnetic probability-current representation, providing a field-equivalence description of parity-mixed charge displacement. In this notation, the total EDM expectation takes the unified form 〈d⃗̂tot〉=dB(gE〈J⃗̂p〉ℏ+gEe〈S⃗̂〉ℏ), with gEe=2dintdB, where J⃗̂p captures Stark-induced pseudoangular momentum and S⃗̂ encodes any intrinsic (spin-aligned) EDM dint from symmetry-violating interactions. We define a natural electric dipole unit (the “Bohr EDM”) as dB≡ea0=2μBcα (a0 the Bohr radius and μB the Bohr magneton). As a canonical analytic benchmark, we show in the hydrogenic problem that a static electric field couples within a fixed n manifold through the scaled Runge-Lenz structure, yielding a compact Landé-like description and reproducing the Stark doublet (e.g., |〈dorb〉|=3dB for the 2s–2pm=0 mixing).

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