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Experimental observation of nonlinear Thomson scattering
Donald Umstadter Publications
  • Szu-yuan Chen, University of Michigan, Ann Arbor, MI
  • Anatoly Maksimchuk, University of Michigan
  • Donald Umstadter, University of Nebraska - Lincoln
Date of this Version
11-5-2006
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Published by arXiv:physics/9810036 v3 28 Oct 1998. Copyright 1998. Permission to use.

Abstract

A century ago, J. J. Thomson showed that the scattering of low-intensity light by electrons was a linear process (i.e., the scattered light frequency was identical to that of the incident light) and that light’s magnetic field played no role. To- day, with the recent invention of ultra-high-peak- power lasers it is now possible to create a sufficient photon density to study Thomson scattering in the relativistic regime. With increasing light intensity, electrons quiver during the scattering process with increasing velocity, approaching the speed of light when the laser intensity approaches 1018 W/cm2. In this limit, the effect of light’s magnetic field on electron motion should become comparable to that of its electric field, and the electron mass should increase because of the relativistic correction. Consequently, electrons in such high fields are predicted to quiver nonlinearly, moving in figure-eight patterns, rather than in straight lines, and thus to radiate photons at harmonics of the frequency of the incident laser light, with each harmonic having its own unique angular distribution. In this letter, we report the first ever direct experimental confirmation of these predictions, a topic that has previously been referred to as nonlinear Thomson scattering. Extension of these results to coherent relativistic harmonic generation may eventually lead to novel table-top x-ray sources.

Citation Information
Szu-yuan Chen, Anatoly Maksimchuk and Donald Umstadter. "Experimental observation of nonlinear Thomson scattering" (2006)
Available at: http://works.bepress.com/donald_umstadter/29/