Topological Currents in Extended Electrodynamics, Negative Effective Dispersion, and Supersymmetric Consistency Constraints

We investigate a proposed extension of four-dimensional electrodynamics in which aclosed three-form current Js ∈ Ω3(X) is constructed from higher-dimensional geometric datathrough fiber integration over a (4 + n)-dimensional bulk bundle Y π−→ X. We distinguishtwo differential-form constructions: the pushforward of even-degree Chern–Weil forms builtfrom the Chern character and the Dirac ˆA-genus (whose square equals the Todd class ofthe complexified vertical bundle, Td(Tπ ⊗ C) = ˆA(Tπ )2) over odd-dimensional real fibers(n = 2m − 1), and the use of odd Chern-character data in K−1(Y ) over even-dimensionalcomplex fibers (n = 2m). For a globally defined gauge potential A ∈ Ω1(X) with fieldstrength F = dA, the coupling A ∧ Js defines a gauge-invariant action yielding the modifiedMaxwell equation d ∗ F = Js alongside dF = 0. Because ∗F is globally defined, d ∗ F = Jsrequires Js to be globally exact ([Js]dR = 0) on X, supporting non-zero charge on boundedspatial regions while having vanishing periods on closed three-cycles; we also outline hownontrivial bundles can be coupled via F ∧ Bs when Js = dBs, and identify defect andhigher-gerbe extensions as directions requiring further construction if [Js]dR̸ = 0.We then examine how a dimension-six higher-spatial-derivative operator, defined relative toa preferred background direction uμ associated with ∗Js and acting selectively on the spatiallyprojected magnetic two-form F ⊥μν , modifies photon dispersion while avoiding additionalhigher-time-derivative modes at the classical level. Within the sub-threshold momentumregime 0 < q < qstab = 1/√β = Λn/√αs (with β = αs/Λ2n in natural units ℏ = c = 1), thetruncated quadratic model exhibits a negative dispersion curvature mass m∗(q) ≃ −1/(3βq) =−Λ2n/(3αsq) < 0 while maintaining a positive canonical quadratic Hamiltonian.Finally, we discuss formal local electric-magnetic dualization, connections with theKapustin–Witten framework, and supersymmetric operator protection. We formulate thesupersymmetry connection as an open research conjecture regarding whether microscopicN ≥ 1 BPS completions protect the spatially projected operator structure against radiativetemporal-derivative mixing, and we derive conditional fixed-energy interferometric phaseshifts and benchmark constraints in terms of the differential arm-to-arm coupling variance.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-29
DOI
https://doi.org/10.5281/zenodo.23766965
Primary Topic
Quantum and Classical Electrodynamics
Type
article
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article

Topological Currents in Extended Electrodynamics, Negative Effective Dispersion, and Supersymmetric Consistency Constraints

peter de ceuster
Zenodo (CERN European Organization for Nuclear Research)
Quantum and Classical Electrodynamics
article

Topological Currents in Extended Electrodynamics, Negative Effective Dispersion, and Supersymmetric Consistency Constraints

peter de ceuster
article en

Abstract

We investigate a proposed extension of four-dimensional electrodynamics in which aclosed three-form current Js ∈ Ω3(X) is constructed from higher-dimensional geometric datathrough fiber integration over a (4 + n)-dimensional bulk bundle Y π−→ X. We distinguishtwo differential-form constructions: the pushforward of even-degree Chern–Weil forms builtfrom the Chern character and the Dirac ˆA-genus (whose square equals the Todd class ofthe complexified vertical bundle, Td(Tπ ⊗ C) = ˆA(Tπ )2) over odd-dimensional real fibers(n = 2m − 1), and the use of odd Chern-character data in K−1(Y ) over even-dimensionalcomplex fibers (n = 2m). For a globally defined gauge potential A ∈ Ω1(X) with fieldstrength F = dA, the coupling A ∧ Js defines a gauge-invariant action yielding the modifiedMaxwell equation d ∗ F = Js alongside dF = 0. Because ∗F is globally defined, d ∗ F = Jsrequires Js to be globally exact ([Js]dR = 0) on X, supporting non-zero charge on boundedspatial regions while having vanishing periods on closed three-cycles; we also outline hownontrivial bundles can be coupled via F ∧ Bs when Js = dBs, and identify defect andhigher-gerbe extensions as directions requiring further construction if [Js]dR̸ = 0.We then examine how a dimension-six higher-spatial-derivative operator, defined relative toa preferred background direction uμ associated with ∗Js and acting selectively on the spatiallyprojected magnetic two-form F ⊥μν , modifies photon dispersion while avoiding additionalhigher-time-derivative modes at the classical level. Within the sub-threshold momentumregime 0 < q < qstab = 1/√β = Λn/√αs (with β = αs/Λ2n in natural units ℏ = c = 1), thetruncated quadratic model exhibits a negative dispersion curvature mass m∗(q) ≃ −1/(3βq) =−Λ2n/(3αsq) < 0 while maintaining a positive canonical quadratic Hamiltonian.Finally, we discuss formal local electric-magnetic dualization, connections with theKapustin–Witten framework, and supersymmetric operator protection. We formulate thesupersymmetry connection as an open research conjecture regarding whether microscopicN ≥ 1 BPS completions protect the spatially projected operator structure against radiativetemporal-derivative mixing, and we derive conditional fixed-energy interferometric phaseshifts and benchmark constraints in terms of the differential arm-to-arm coupling variance.

Zenodo (CERN European Organization for Nuclear Research)
Openalex Percentile: Top 20%
Quantum and Classical Electrodynamics
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Topological Currents in Extended Electrodynamics, Negative Effective Dispersion, and Supersymmetric Consistency Constraints — peter de ceuster · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS