Short Rayleigh length free electron lasers

Conventional free electron laser (FEL) oscillators minimize the optical mode volume around the electron beam in the undulator by making the resonator Rayleigh length about one third to one half of the undulator length. This maximizes gain and beam-mode coupling. In compact configurations of high-pow...

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Main Authors: W. B. Colson, J. Blau, R. L. Armstead, P. P. Crooker, R. Vigil, T. Voughs, B. W. Williams
Format: Article
Language:English
Published: American Physical Society 2006-03-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.9.030703
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spelling doaj-070466095e9843b59c4db5829006dbaa2020-11-25T00:16:48ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022006-03-019303070310.1103/PhysRevSTAB.9.030703Short Rayleigh length free electron lasersW. B. ColsonJ. BlauR. L. ArmsteadP. P. CrookerR. VigilT. VoughsB. W. WilliamsConventional free electron laser (FEL) oscillators minimize the optical mode volume around the electron beam in the undulator by making the resonator Rayleigh length about one third to one half of the undulator length. This maximizes gain and beam-mode coupling. In compact configurations of high-power infrared FELs or moderate power UV FELs, the resulting optical intensity can damage the resonator mirrors. To increase the spot size and thereby reduce the optical intensity at the mirrors below the damage threshold, a shorter Rayleigh length can be used, but the FEL interaction is significantly altered. We model this interaction using a coordinate system that expands with the rapidly diffracting optical mode from the ends of the undulator to the mirrors. Simulations show that the interaction of the strongly focused optical mode with a narrow electron beam inside the undulator distorts the optical wave front so it is no longer in the fundamental Gaussian mode. The simulations are used to study how mode distortion affects the single-pass gain in weak fields, and the steady-state extraction in strong fields.http://doi.org/10.1103/PhysRevSTAB.9.030703
collection DOAJ
language English
format Article
sources DOAJ
author W. B. Colson
J. Blau
R. L. Armstead
P. P. Crooker
R. Vigil
T. Voughs
B. W. Williams
spellingShingle W. B. Colson
J. Blau
R. L. Armstead
P. P. Crooker
R. Vigil
T. Voughs
B. W. Williams
Short Rayleigh length free electron lasers
Physical Review Special Topics. Accelerators and Beams
author_facet W. B. Colson
J. Blau
R. L. Armstead
P. P. Crooker
R. Vigil
T. Voughs
B. W. Williams
author_sort W. B. Colson
title Short Rayleigh length free electron lasers
title_short Short Rayleigh length free electron lasers
title_full Short Rayleigh length free electron lasers
title_fullStr Short Rayleigh length free electron lasers
title_full_unstemmed Short Rayleigh length free electron lasers
title_sort short rayleigh length free electron lasers
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2006-03-01
description Conventional free electron laser (FEL) oscillators minimize the optical mode volume around the electron beam in the undulator by making the resonator Rayleigh length about one third to one half of the undulator length. This maximizes gain and beam-mode coupling. In compact configurations of high-power infrared FELs or moderate power UV FELs, the resulting optical intensity can damage the resonator mirrors. To increase the spot size and thereby reduce the optical intensity at the mirrors below the damage threshold, a shorter Rayleigh length can be used, but the FEL interaction is significantly altered. We model this interaction using a coordinate system that expands with the rapidly diffracting optical mode from the ends of the undulator to the mirrors. Simulations show that the interaction of the strongly focused optical mode with a narrow electron beam inside the undulator distorts the optical wave front so it is no longer in the fundamental Gaussian mode. The simulations are used to study how mode distortion affects the single-pass gain in weak fields, and the steady-state extraction in strong fields.
url http://doi.org/10.1103/PhysRevSTAB.9.030703
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