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Lienard-Wiechert potentials and synchrotron radiation from a relativistic spinning particle in pseudoclassical theory

  • Elementary Particles and Fields
  • Theory
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Abstract

For a relativistic spinning particle with an anomalous magnetic moment, Lienard-Wiechert potentials are constructed within the pseudoclassical approach. Some specific cases of the motion of a spinning particle are considered on the basis of general expressions obtained in this study for the Lienard-Wiechert potentials. In particular, the intensity of the synchrotron radiation from a transversely polarized particle moving along a circle at a constant speed is investigated as a function of the particle spin. In the specific case of particles having no anomalous magnetic moment and moving in an external uniform magnetic field, the resulting expressions coincide with familiar formulas from the quantum theory of radiation. The spin dependence of the polarization of synchrotron radiation is investigated.

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Translated from Yadernaya Fizika, Vol. 63, No. 12, 2000, pp. 2211–2218.

Original Russian Text Copyright © 2000 by Arakelyan, G. Grigoryan, R. Grigoryan.

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Arakelyan, S.A., Grigoryan, G.V. & Grigoryan, R.P. Lienard-Wiechert potentials and synchrotron radiation from a relativistic spinning particle in pseudoclassical theory. Phys. Atom. Nuclei 63, 2115–2122 (2000). https://doi.org/10.1134/1.1333882

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  • DOI: https://doi.org/10.1134/1.1333882

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