Magnetic Monopole Decay and Its Consequences

dc.creatorFrankel, S.
dc.date1999-06-15
dc.date.accessioned2026-07-07T05:43:08Z
dc.date.available2026-07-07T05:43:08Z
dc.descriptionWe 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)/r^3, as well as the Dirac angular momentum, vec(l_f) = 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.
dc.descriptionuuencoded files, 10 pages
dc.identifierhttps://arxiv.org/abs/nucl-th/9906043
dc.identifierhttp://arxiv.org/abs/nucl-th/9906043
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/83194
dc.subjectNuclear Theory
dc.subjectHigh Energy Physics - Theory
dc.titleMagnetic Monopole Decay and Its Consequences
dc.typetext

Files

Collections