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Magnetic Monopole Decay and Its Consequences

1999/06/15 by S. Frankel, Frankel, S.
Biochemistry, Genetics and Molecular Biology · Materials Science · Physics and Astronomy · #FOS: Physical sciences #Geomagnetism and Paleomagnetism Studies #High Energy Physics - Theory (hep-th) #Magnetic Properties of Alloys #Nuclear Theory (nucl-th) #hep-th #nucl-th

paper · pdf · doi:10.48550/arxiv.nucl-th/9906043

uuencoded files, 10 pages

arxiv created 1999/06/15 · openalex publication_date 1999/06/15 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We return to further examination of the need for the existence of magnetic monopoles based on the decades old derivation [Sherman Frankel, Amer. Jour. of Physics, 44, 7, 683-6 1976], of both the monopole-charge force, vec(F) = eg(vec(r) * vec(v)/c)/r3, as well as the Dirac angular momentum, vec(lf) = eg hat(r), from P and T conservation alone, without any recourse whatsoever to Maxwell's Equations. The eg product also appeared in the charge conserving equation, deg/dt = 0 = edg/dt + gde/dt, and this paper examines the second possible solution, dg/dt = - de/dt, namely monopole decay, accounting for the non-observance of stable monopoles. It treats astrophysics and neutrino physics consequences and suggestions for experimental searches.

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