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Lettere al Nuovo Cimento (1971-1985)

, Volume 35, Issue 15, pp 455–456 | Cite as

Electromagnetic field of a rotating closed singular magnetic flux line and of a distribution of those corresponding to a bohr-magneton dipole

  • H. Jehle
Article
  • 17 Downloads

Summary

The field lines (Faraday lines) of a magnetic dipole may be understood in terms of a superposition of a manifold (of alternative forms) of closed loops of quantized magnetic flux, in a manner similar to a Feynman probability amplitude super-position of alternative path histories. This manifold represents a statistical distribution over azimuth and size of Faraday field-line loops, corresponding to a density of lines which represents 〈B〉 ∝ μr-3. It is pointed out that, with μ =/2mc (Bohr magneton), and with the spin being represented by a Zitterbewegung angular velocity 2mc2/ħ of the entire loop manifold, the magnetic field implies, by the basic relativistic definitionAμ = (ħc/e)∂μθ (θ = electromagnetic gauge variable) for quantized flux, also an electric field 〈E〉 ∝er-2.

Pacs

12.20 Electromagnetic and unified gauge fields 

Copyright information

© Società Italiana di Fisica 1982

Authors and Affiliations

  • H. Jehle
    • 1
  1. 1.Sektion Physik Universität MünchenMünchen 2

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