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A review of free‐electron lasers

C. W. Roberson, +1 more
- 01 Jan 1989 - 
- Vol. 1, Iss: 1, pp 3-42
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TLDR
In this paper, the physical mechanism responsible for the generation of coherent radiation in the FEL is described and the fundamental role of the ponderomotive wave in bunching and trapping the beam is emphasized.
Abstract
Free‐electron laser (FEL) theory and experiments are reviewed. The physical mechanism responsible for the generation of coherent radiation in the FEL is described and the fundamental role of the ponderomotive wave in bunching and trapping the beam is emphasized. The relationship of the FEL interaction to the beam–plasma interaction is pointed out. Various FEL operating regimes are discussed. These include the high‐gain Compton and Raman regimes, both with and without an axial guiding magnetic field. The linear and nonlinear regimes are examined in detail, with particular emphasis on techniques for achieving efficiency enhancement. The quality of the electron beam used to drive FEL’s is a critical factor in determining their gain and efficiency. The subject of electron beam quality, for different accelerators, is discussed. Key proof‐of‐principle experiments for FELs in an axial guiding magnetic field, as well as those driven by induction linacs, rf linacs, electrostatic accelerators, and storage rings, are reviewed. Finally, the requirements on wigglers and resonators are discussed.

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Citations
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Interaction of ultra-high laser fields with beams and plasmas

TL;DR: The nonlinear interaction of ultraintense laser pulses with electron beams and plasmas is rich in a wide variety of new phenomena as discussed by the authors, including laser excitation of large-amplitude plasma waves (wake fields), relativistic optical guiding of laser pulses in preformed plasma channels, laser frequency amplification by ionization fronts and plasma waves, and stimulated backscattering from plasma and electron beams, and cooling of electron beams by intense lasers.
Journal ArticleDOI

Interaction of ultrahigh laser fields with beams and plasmas

TL;DR: The nonlinear interaction of ultraintense laser pulses with electron beams and plasmas is rich in a wide variety of new phenomena as discussed by the authors, including laser excitation of large-amplitude plasma waves (wake fields), relativistic optical guiding of laser pulses in preformed plasma channels, laser frequency amplification by ionization fronts and plasma waves, and stimulated backscattering from plasma and electron beams, and cooling of electron beams by intense lasers.
Journal ArticleDOI

Nonlinear Thomson scattering: A tutorial

TL;DR: In this article, the classical theory of nonlinear Thomson scattering of an electron in an intense laser field is presented, and simple asymptotic expansions are obtained for the spectrum of radiation that is backscattered from a laser by a counter-propagating (or co-proposing) electron.

Observation of single-mode operation in a free-electron laser. Technical report, 1 October 1985-30 December 1986

L.R. Elias, +3 more
TL;DR: Time-structure and frequency-spectrum measurements of the UC Santa Barbara free-electron-laser oscillator show that for periods shorter than 5 microsec, the laser-frequency changes in unexpected quantized steps, which may be explained in terms of a homogeneously broadened gain profile coupled to a small monotonic drift in electron-beam energy.
References
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Journal ArticleDOI

Collective instabilities and high-gain regime in a free electron laser

TL;DR: In this article, the behavior of a free electron laser in the high gain regime and the conditions for the emergence of a collective instability in the electron beam-undulator-field system were studied.
Journal ArticleDOI

Stimulated Emission of Bremsstrahlung in a Periodic Magnetic Field

TL;DR: In this paper, the Weizsacker-Williams method is used to calculate the gain due to the induced emission of radiation into a single electromagnetic mode parallel to the motion of a relativistic electron through a periodic transverse dc magnetic field.
Journal ArticleDOI

First Operation of a Free-Electron Laser

TL;DR: A free-electron laser oscillator has been operated above threshold at a wavelength of 3.4 µm as discussed by the authors, where µm is the number of free electrons in a single photon.
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