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Research PaperResearchia:202604.29017

Effective Observer-Split Source Terms in Rotating Frames and Gravitomagnetic Backgrounds in Extended Aharonov-Bohm Electrodynamics

A. Iadicicco

Abstract

We examine whether rotating frames and stationary gravitomagnetic backgrounds can provide a meaningful link to extended Aharonov-Bohm electrodynamics without invoking microscopic charge non-conservation. For standard generally covariant, locally $U(1)$-invariant matter, the answer at the microscopic level is negative: the physical four-current remains covariantly conserved, so neither rotation nor stationary gravitomagnetism by themselves generate a genuine source for the scalar sector. A weaker...

Submitted: April 29, 2026Subjects: Physics; Physics

Description / Details

We examine whether rotating frames and stationary gravitomagnetic backgrounds can provide a meaningful link to extended Aharonov-Bohm electrodynamics without invoking microscopic charge non-conservation. For standard generally covariant, locally U(1)U(1)-invariant matter, the answer at the microscopic level is negative: the physical four-current remains covariantly conserved, so neither rotation nor stationary gravitomagnetism by themselves generate a genuine source for the scalar sector. A weaker but still useful connection nevertheless emerges after a 3+13+1 decomposition with respect to a rotating observer congruence. In that description, the observer-measured transport current on the spatial slice obeys a projected continuity equation containing an exact split source term Isplit1NDi(ρβi)I_{\mathrm{split}} \equiv \frac{1}{N} D_i(ρ\,β^i), which reduces in the weak-field regime to IG=Di(ρβi)I_G = D_i(ρ\,β^i). This term is not a frame-independent microscopic anomaly; it is the bookkeeping term that appears when covariant conservation is rewritten in transport variables adapted to a rotating slicing. We then propose a phenomenological AB-type closure in which this split source drives the scalar sector on finite-scale rotating systems. In the rigid-rotation weak-field limit, the source reduces to IG=(Ω×r)ρI_G = (\boldsymbolΩ \times \mathbf{r})\cdot \nabla ρ, and for localized transients to IG=Ωφ(δρs) I_G = Ω\partial_φ(δρ_s). The resulting framework is therefore effective rather than fundamental, observer-tied rather than local-inertial, and experimentally meaningful only at mesoscopic or macroscopic scales. It yields concrete operational signatures, including reversal under ΩΩΩ\to -Ω, suppression for nearly axisymmetric charge distributions, and sensitivity to transient non-axisymmetric charge structure.


Source: arXiv:2604.24787v1 - http://arxiv.org/abs/2604.24787v1 PDF: https://arxiv.org/pdf/2604.24787v1 Original Link: http://arxiv.org/abs/2604.24787v1

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Date:
Apr 29, 2026
Topic:
Physics
Area:
Physics
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