2017
DOI: 10.1103/physrevaccelbeams.20.020701
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Compact beam transport system for free-electron lasers driven by a laser plasma accelerator

Abstract: Utilizing laser-driven plasma accelerators (LPAs) as a high-quality electron beam source is a promising approach to significantly downsize the x-ray free-electron laser (XFEL) facility. A multi-GeV LPA beam can be generated in several-centimeter acceleration distance, with a high peak current and a low transverse emittance, which will considerably benefit a compact FEL design. However, the large initial angular divergence and energy spread make it challenging to transport the beam and realize FEL radiation. In… Show more

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Cited by 27 publications
(19 citation statements)
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“…Dispersion effects on performance of free-electron laser based on laser wakefield accelerator We attempt to perform the EUV FEL operation by employing the attainable LWFA beam parameters from Shanghai Institute of Optics and Fine Mechanics (SIOM) [17,28,29] and the compact beam transport system considered in Ref. [30]. The parameters for the e beam at the entrance of the undulator are shown in Table 1.…”
Section: Dispersion Effects On Fel Radiationmentioning
confidence: 99%
“…Dispersion effects on performance of free-electron laser based on laser wakefield accelerator We attempt to perform the EUV FEL operation by employing the attainable LWFA beam parameters from Shanghai Institute of Optics and Fine Mechanics (SIOM) [17,28,29] and the compact beam transport system considered in Ref. [30]. The parameters for the e beam at the entrance of the undulator are shown in Table 1.…”
Section: Dispersion Effects On Fel Radiationmentioning
confidence: 99%
“…A TGU with a transverse magnetic field variation was initially proposed to improve FEL performance of an electron beam with a large energy spread [21,22] and being tested for FEL driven by laser plasma accelerator [23]. In this study, we make use of the dispersion generated by a TGU.…”
Section: A Beam Dynamics Of a Tgumentioning
confidence: 99%
“…ρ is normally of the orders of 10 −3 , so this condition is not acomplished by typical LPA beams since energy spreads have been measured to be~10 −2 for MeV-GeV [18]. In order to use these beams for FEL, the energy spread should be reduced, for example, by cutting a part of the initial distribution using a demixing chicane to select a smaller range of energies [19] or take advantage of the energy spread by opting for a different approach with the use of transverse gradient undulators (TGUs) [20,21]. The FEL amplification highly depends on the overlapping of the electron beam and the wave.…”
mentioning
confidence: 99%