The Self-Force of a Charged Particle in Classical Electrodynamics with a Cut-off

Simple item page
dc.creatorFrenkel, Josif
dc.creatorSantos, R B
dc.date1998-07-29
dc.date.accessioned2026-07-07T07:39:13Z
dc.date.available2026-07-07T07:39:13Z
dc.descriptionWe discuss, in the context of classical electrodynamics with a Lorentz invariant cut-off at short distances, the self-force acting on a point charged particle. It follows that the electromagnetic mass of the point charge occurs in the equation of motion in a form consistent with special relativity. We find that the exact equation of motion does not exhibit runaway solutions or non-causal behavior, when the cut-off is larger than half of the classical radius of the electron.
dc.description17 pages, 1 figure
dc.identifierhttps://arxiv.org/abs/physics/9807054
dc.identifierhttp://arxiv.org/abs/physics/9807054
dc.identifierInt.J.Mod.Phys. B13 (1999) 315-324
dc.identifierdoi:10.1142/S0217979299000199
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/121366
dc.subjectClassical Physics
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Theory
dc.titleThe Self-Force of a Charged Particle in Classical Electrodynamics with a Cut-off
dc.typetext

Files

Collections

arXiv