Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler

Free-electron laser amplifiers have been operated at high efficiency at wavelengths from the microwave through the visible. Typically, these amplifiers require long tapered sections and produce spent beams with large energy spreads that are 4–5 times the electronic efficiency. In addition, while opt...

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Main Author: H. P. Freund
Format: Article
Language:English
Published: American Physical Society 2013-06-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.16.060701
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spelling doaj-c251d6ad6d504c75980d1d9ca1db6f112020-11-25T02:46:54ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022013-06-0116606070110.1103/PhysRevSTAB.16.060701Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wigglerH. P. FreundFree-electron laser amplifiers have been operated at high efficiency at wavelengths from the microwave through the visible. Typically, these amplifiers require long tapered sections and produce spent beams with large energy spreads that are 4–5 times the electronic efficiency. In addition, while optical guiding during exponential growth in the uniform wiggler section confines the optical mode, the guiding disappears in the tapered wiggler section resulting in a relatively large optical mode at the wiggler exit. Optical klystrons consist of a Modulator wiggler that induces a velocity modulation on the electron beam followed by a magnetic dispersive section that enhances the velocity modulation prior to injection into a second, radiator wiggler. Optical klystrons have been operated over a broad spectral range; however, no optical klystron has been built with a tapered radiator wiggler. A comparison between a optical klystron with a step-tapered Radiator wiggler and a conventional tapered wiggler amplifier is analyzed in this paper. The purpose of the step taper is to both enhance the efficiency and to extend the range of the exponential gain and so preserve the optical guiding over a longer interaction length. The step-tapered optical klystron and a tapered wiggler amplifier are compared for a nominal set of parameters to determine the differences in the efficiency, interaction length, spent beam energy spread, and the size of the optical mode at the wiggler exit.http://doi.org/10.1103/PhysRevSTAB.16.060701
collection DOAJ
language English
format Article
sources DOAJ
author H. P. Freund
spellingShingle H. P. Freund
Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
Physical Review Special Topics. Accelerators and Beams
author_facet H. P. Freund
author_sort H. P. Freund
title Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
title_short Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
title_full Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
title_fullStr Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
title_full_unstemmed Comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
title_sort comparison of free-electron laser amplifiers based on a step-tapered optical klystron and a conventional tapered wiggler
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2013-06-01
description Free-electron laser amplifiers have been operated at high efficiency at wavelengths from the microwave through the visible. Typically, these amplifiers require long tapered sections and produce spent beams with large energy spreads that are 4–5 times the electronic efficiency. In addition, while optical guiding during exponential growth in the uniform wiggler section confines the optical mode, the guiding disappears in the tapered wiggler section resulting in a relatively large optical mode at the wiggler exit. Optical klystrons consist of a Modulator wiggler that induces a velocity modulation on the electron beam followed by a magnetic dispersive section that enhances the velocity modulation prior to injection into a second, radiator wiggler. Optical klystrons have been operated over a broad spectral range; however, no optical klystron has been built with a tapered radiator wiggler. A comparison between a optical klystron with a step-tapered Radiator wiggler and a conventional tapered wiggler amplifier is analyzed in this paper. The purpose of the step taper is to both enhance the efficiency and to extend the range of the exponential gain and so preserve the optical guiding over a longer interaction length. The step-tapered optical klystron and a tapered wiggler amplifier are compared for a nominal set of parameters to determine the differences in the efficiency, interaction length, spent beam energy spread, and the size of the optical mode at the wiggler exit.
url http://doi.org/10.1103/PhysRevSTAB.16.060701
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