1999
DOI: 10.1103/physreva.60.785
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Relativistic dynamics of charges in electromagnetic fields: An eigenspinor approach

Abstract: Analytical solutions and fresh insights for the relativistic dynamics of charges in classical electromagnetic fields are made possible by an eigenspinor approach. The Lorentz-force equation takes a simple spinorial form when expressed in terms of an amplitude of the Lorentz transformation that describes the motion of the charge in Clifford's geometric algebra of physical space. Algebraic projectors allow explicit analytical solutions to be found for charges in arbitrary initial motion interacting with monochro… Show more

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Cited by 30 publications
(26 citation statements)
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“…Solutions can also be found for relativistic charge motion in plane waves [19], plane-wave pulses, or plane waves superimposed on static longitudinal electric or magnetic fields [6,20].…”
Section: Eigenspinorsmentioning
confidence: 99%
“…Solutions can also be found for relativistic charge motion in plane waves [19], plane-wave pulses, or plane waves superimposed on static longitudinal electric or magnetic fields [6,20].…”
Section: Eigenspinorsmentioning
confidence: 99%
“…However, together with the requirements 6) this does give a consistent set, and it is completely symmetric on all events whose distance from an arbitrary origin O remains finite. In other words, the assymetry is restricted to and directly related with the structure at infinity itself.…”
Section: The Cga 7 Model For Spacetimementioning
confidence: 99%
“…This technique allows one to solve the equations with considerable ease in a number of interesting cases such as the motion of charges in constant electromagnetic fields, the Coulomb potential and in electromagnetic planewaves [6]. Usually it is the position dependence of F that presents problems when one wants to fully exploit the nice linearity of the equations.…”
Section: Introductionmentioning
confidence: 99%
“…However, isotopic pairs of particles can be isolated in the spinor by applying primitive idempotents on the right, and such projected spinors do belong to distinct minimal left ideals. The transformation behaviour is determined by the geometric role of the spinor [1,15,16] as an amplitude of the Lorentz transformation relating a reference frame for the particles to the lab frame: the spinor is subject to independent transformations on the right and left. It is through this structure, together with the Minkowskian metric of paravector space [4], that we are able to model all the fermions of a generation in just seven spatial (eight spacetime) dimensions with an algebra represented by 8 × 8 matrices.…”
Section: Introductionmentioning
confidence: 99%