Abstract

The equations of motion for the relativistic particle in an external electromagnetic field are reformulated within the framework of the Nambu three-order phase space formalism. This formulation implies the mass of a relativistic particle as an integral of motion. The Lorentz-covariant four-vector of momentum is decomposed into two four-dimensional euclidean vectors forming the coordinates of the three-order phase space formalism. The new set of equations of motion describing the motion of a relativistic charged spinning particle in interaction with an external electromagnetic field is given in terms of quaternions. These equations give rise to Lorentz-force equations with no auxiliary conditions.

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