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Quasilinear theory of radiation saturation in a free-electron laser

Journal Article · · Journal of Applied Physics; (USA)
DOI:https://doi.org/10.1063/1.345308· OSTI ID:6900550
 [1];  [2]
  1. University of Maryland, Department of Physics and Astronomy, College Park, Maryland 20742 (USA)
  2. Plasma Physics Division, Naval Research Laboratory, Washington, DC 20375 (USA)

A quasilinear theory of the self-consistent evolution of the electron-beam distribution and radiation field within a free-electron laser is presented. The relativistic electron beam propagates through an ideal helical wiggler {bold B}{sub 0}={minus}{ital B}{sub {ital w}}(cos {ital k}{sub {ital w}}{ital z}{ital {cflx e}}{sub {ital x}}+sin {ital k}{sub {ital w}}{ital z}{ital {cflx e}}{sub {ital y}}), for which the transverse gradients {partial derivative}/{partial derivative}{ital x}=0={partial derivative}/{partial derivative}{ital y} have been neglected. The transverse variation of both the transverse-polarized radiation field and the electron-beam distribution have also been neglected. Additionally, the electron beam is assumed to be sufficiently tenuous that the longitudinal space-charge potential {delta}{phi} is negligible and the Compton approximations are applicable. The resulting asymptotic expression for the spectral energy density is used to evaluate the efficiency and saturated radiation power in a variety of parameter regimes relevant to experiments.

OSTI ID:
6900550
Journal Information:
Journal of Applied Physics; (USA), Journal Name: Journal of Applied Physics; (USA) Vol. 67:8; ISSN 0021-8979; ISSN JAPIA
Country of Publication:
United States
Language:
English