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Main Author: Tobar, Michael E.
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2511.07692
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author Tobar, Michael E.
author_facet Tobar, Michael E.
contents EDMs probe fundamental symmetries and underpin BSM searches. We give a symmetry-based description, analogous to the Zeeman effect, that puts magnetic and electric dipoles on equal footing under EM duality. In hydrogen, $\vec B$ (pseudovector) couples to $\hat{\vec J}$ and reduces $SO(4)$ to $SO(2)$ generated by $\hat J_z$. A static $\vec E$ (polar) couples within a fixed $n$ to a scaled Runge-Lenz operator $\hat{\vec A}_{\rm sc}$, mixes parities, and preserves $SO(2)\times SO(2)$ generated by $\hat J_z$ and $\hat A_{{\rm sc},z}$. This motivates a pseudo-angular momentum $\hat{\vec J}_p$ built from $\hat{\vec A}_{\rm sc}$ and a Landé factor $g_E$, so the orbital dipole is $\hat{\vec d}_{\rm orb}=g_E d_B \hat{\vec J}_p/\hbar$, with $d_B=ea_0=2μ_B/(cα)$. Stark mixing of $2s$ and $2p_{m=0}$ gives $|\langle d_{\rm orb}\rangle|=3d_B$ ($g_E=3$). Following Ohanian's magnetisation formalism, we construct its electric dual: the microscopic polarisation $\vec P$ has nonzero curl, defining a magnetic probability current $\vec J_m=-ε_0^{-1}\nabla\times\vec P$, and the EDM expectation is $\langle \hat{\vec d}_{\rm tot}\rangle=-\frac{ε_0}{2}\int \vec r\times \vec J_m\, d^3r=d_B\big[g_E\langle \hat{\vec J}_p\rangle/\hbar+g_E^{e}\langle \hat{\vec S}\rangle/\hbar\big]$, with $g_E^{e}=2d_{\rm int}/d_B$. Here $\hat{\vec S}$ encodes any intrinsic EDM $d_{\rm int}$, while $\hat{\vec J}_p$ captures the Stark-induced pseudo-angular momentum from Runge-Lenz symmetry. The dual framework shows that induced EDMs may be described by circulating magnetic probability currents, mirroring magnetic dipoles from circulating electric probability currents.
format Preprint
id arxiv_https___arxiv_org_abs_2511_07692
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Dual Magnetic and Electric Dipole Symmetry: Pseudo Angular Momentum in Parity Space and the Electric Landé $g$-Factor
Tobar, Michael E.
Atomic Physics
Quantum Physics
EDMs probe fundamental symmetries and underpin BSM searches. We give a symmetry-based description, analogous to the Zeeman effect, that puts magnetic and electric dipoles on equal footing under EM duality. In hydrogen, $\vec B$ (pseudovector) couples to $\hat{\vec J}$ and reduces $SO(4)$ to $SO(2)$ generated by $\hat J_z$. A static $\vec E$ (polar) couples within a fixed $n$ to a scaled Runge-Lenz operator $\hat{\vec A}_{\rm sc}$, mixes parities, and preserves $SO(2)\times SO(2)$ generated by $\hat J_z$ and $\hat A_{{\rm sc},z}$. This motivates a pseudo-angular momentum $\hat{\vec J}_p$ built from $\hat{\vec A}_{\rm sc}$ and a Landé factor $g_E$, so the orbital dipole is $\hat{\vec d}_{\rm orb}=g_E d_B \hat{\vec J}_p/\hbar$, with $d_B=ea_0=2μ_B/(cα)$. Stark mixing of $2s$ and $2p_{m=0}$ gives $|\langle d_{\rm orb}\rangle|=3d_B$ ($g_E=3$). Following Ohanian's magnetisation formalism, we construct its electric dual: the microscopic polarisation $\vec P$ has nonzero curl, defining a magnetic probability current $\vec J_m=-ε_0^{-1}\nabla\times\vec P$, and the EDM expectation is $\langle \hat{\vec d}_{\rm tot}\rangle=-\frac{ε_0}{2}\int \vec r\times \vec J_m\, d^3r=d_B\big[g_E\langle \hat{\vec J}_p\rangle/\hbar+g_E^{e}\langle \hat{\vec S}\rangle/\hbar\big]$, with $g_E^{e}=2d_{\rm int}/d_B$. Here $\hat{\vec S}$ encodes any intrinsic EDM $d_{\rm int}$, while $\hat{\vec J}_p$ captures the Stark-induced pseudo-angular momentum from Runge-Lenz symmetry. The dual framework shows that induced EDMs may be described by circulating magnetic probability currents, mirroring magnetic dipoles from circulating electric probability currents.
title Dual Magnetic and Electric Dipole Symmetry: Pseudo Angular Momentum in Parity Space and the Electric Landé $g$-Factor
topic Atomic Physics
Quantum Physics
url https://arxiv.org/abs/2511.07692