X-band rf driven free electron laser driver with optics linearization

In this paper, a compact hard X-ray free electron lasers (FEL) design is proposed with all X-band rf acceleration and two stage bunch compression. It eliminates the need of a harmonic rf linearization section by employing optics linearization in its first stage bunch compression. Quadrupoles and sex...

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Main Authors: Yipeng Sun (孙一鹏), Paul Emma, Tor Raubenheimer, Juhao Wu
Format: Article
Language:English
Published: American Physical Society 2014-11-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.17.110703
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spelling doaj-1f8a0fb0386f48cda4b57bd79f6a2bb32020-11-25T00:53:19ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022014-11-01171111070310.1103/PhysRevSTAB.17.110703X-band rf driven free electron laser driver with optics linearizationYipeng Sun (孙一鹏)Paul EmmaTor RaubenheimerJuhao WuIn this paper, a compact hard X-ray free electron lasers (FEL) design is proposed with all X-band rf acceleration and two stage bunch compression. It eliminates the need of a harmonic rf linearization section by employing optics linearization in its first stage bunch compression. Quadrupoles and sextupoles are employed in a bunch compressor one (BC1) design, in such a way that second order longitudinal dispersion of BC1 cancels the second order energy correlation in the electron beam. Start-to-end 6-D simulations are performed with all the collective effects included. Emittance growth in the horizontal plane due to coherent synchrotron radiation is investigated and minimized, to be on a similar level with the successfully operating Linac coherent light source (LCLS). At a FEL radiation wavelength of 0.15 nm, a saturation length of 40 meters can be achieved by employing an undulator with a period of 1.5 cm. Without tapering, a FEL radiation power above 10 GW is achieved with a photon pulse length of 50 fs, which is LCLS-like performance. The overall length of the accelerator plus undulator is around 250 meters which is much shorter than the LCLS length of 1230 meters. That makes it possible to build hard X-ray FEL in a laboratory with limited size.http://doi.org/10.1103/PhysRevSTAB.17.110703
collection DOAJ
language English
format Article
sources DOAJ
author Yipeng Sun (孙一鹏)
Paul Emma
Tor Raubenheimer
Juhao Wu
spellingShingle Yipeng Sun (孙一鹏)
Paul Emma
Tor Raubenheimer
Juhao Wu
X-band rf driven free electron laser driver with optics linearization
Physical Review Special Topics. Accelerators and Beams
author_facet Yipeng Sun (孙一鹏)
Paul Emma
Tor Raubenheimer
Juhao Wu
author_sort Yipeng Sun (孙一鹏)
title X-band rf driven free electron laser driver with optics linearization
title_short X-band rf driven free electron laser driver with optics linearization
title_full X-band rf driven free electron laser driver with optics linearization
title_fullStr X-band rf driven free electron laser driver with optics linearization
title_full_unstemmed X-band rf driven free electron laser driver with optics linearization
title_sort x-band rf driven free electron laser driver with optics linearization
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2014-11-01
description In this paper, a compact hard X-ray free electron lasers (FEL) design is proposed with all X-band rf acceleration and two stage bunch compression. It eliminates the need of a harmonic rf linearization section by employing optics linearization in its first stage bunch compression. Quadrupoles and sextupoles are employed in a bunch compressor one (BC1) design, in such a way that second order longitudinal dispersion of BC1 cancels the second order energy correlation in the electron beam. Start-to-end 6-D simulations are performed with all the collective effects included. Emittance growth in the horizontal plane due to coherent synchrotron radiation is investigated and minimized, to be on a similar level with the successfully operating Linac coherent light source (LCLS). At a FEL radiation wavelength of 0.15 nm, a saturation length of 40 meters can be achieved by employing an undulator with a period of 1.5 cm. Without tapering, a FEL radiation power above 10 GW is achieved with a photon pulse length of 50 fs, which is LCLS-like performance. The overall length of the accelerator plus undulator is around 250 meters which is much shorter than the LCLS length of 1230 meters. That makes it possible to build hard X-ray FEL in a laboratory with limited size.
url http://doi.org/10.1103/PhysRevSTAB.17.110703
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