RELATIVISTIC FREE-ELECTRON DYNAMICS AND LIGHT-EMISSION SPECTRA IN THESIMULTANEOUS PRESENCE OF A SUPERINTENSE LASER FIELD AND A STRONG UNIFORM MAGNETIC-FIELD

Citation
Yi. Salamin et Fhm. Faisal, RELATIVISTIC FREE-ELECTRON DYNAMICS AND LIGHT-EMISSION SPECTRA IN THESIMULTANEOUS PRESENCE OF A SUPERINTENSE LASER FIELD AND A STRONG UNIFORM MAGNETIC-FIELD, Physical review. A, 58(4), 1998, pp. 3221-3234
Citations number
15
Categorie Soggetti
Physics
Journal title
ISSN journal
10502947
Volume
58
Issue
4
Year of publication
1998
Pages
3221 - 3234
Database
ISI
SICI code
1050-2947(1998)58:4<3221:RFDALS>2.0.ZU;2-Z
Abstract
We present exact analytic trajectories for a relativistic electron in the presence of an elliptically polarized superintense laser field and a strong uniform magnetic field. Also derived are expressions for the velocity components of the electron and for its energy as functions o f the phase of the laser field as a parameter. The analytic trajectory solutions are illustrated by numerical calculations employing laser-f ield parameters and magnetic-field strengths currently available for l aboratory experiments. The trajectory solutions are useful for (among other things) the study of the related problem of emission of radiatio n in the combined laser and magnetic fields. An exact expression for t he cross section of light scattered by an electron initially moving al ong the laser propagation direction and in a magnetic field is given. It is found that, for observation along the common direction of laser propagation and the magnetic field, light at two frequencies omega=ome ga(0) and Omega(0) is scattered, where Omega(0) = gamma(0) (1 + beta(0 )) omega(c), omega(c) is the cyclotron frequency of the electron motio n in the magnetic field, beta(0) is the initial speed of the electron normalized by the speed of light, gamma(0) = (1 - beta(0)(2))(-) (1/2) , and omega(0) is the laser frequency. Using the analytic solutions, w e also study numerically the spectrum of radiation emitted along obser vation directions parallel to the electric and parallel to the magneti c components of the laser field. In each case, we present and discuss the dependence of the spectra on (a) the increase of the electron init ial velocity, (b) the intensity and the frequency of the laser, and (c ) the strength of the magnetic field. [S1050-2947(98)09409-8].