2018
DOI: 10.1016/j.nima.2017.12.005
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Bandwidth broadening of X-ray free electron laser pulses with the natural gradient of planar undulator

Abstract: Besides the target to pursue the narrow bandwidth X-ray pulses, the large bandwidth freeelectron laser pulses are also strongly demanded to satisfy a wide range of scientific user experiments.In this paper, using the transversely tilt beam enabled by deflecting cavity and/or corrugated structure, the potential of large bandwidth X-ray free-electron lasers generation with the natural gradient of the planar undulator are discussed. Simulations confirm the theoretical prediction, and X-ray free-electron laser ban… Show more

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Cited by 8 publications
(9 citation statements)
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“…Two primary methods exist to generate a large-bandwidth free electron laser. One is to use an energy-chirped electron beam [12][13][14]28], and the other is to utilize space-field correlations in the undulator, such as by injecting a head-to-tail tilted beam into a transverse gradient undulator (TGU) [15] or a planar undulator [11]. Using a large energy-chirped electron beam is a simple and natural way to generate broadband XFEL radiation.…”
Section: Broadband Fel Pulse Generation In Sxfelmentioning
confidence: 99%
See 1 more Smart Citation
“…Two primary methods exist to generate a large-bandwidth free electron laser. One is to use an energy-chirped electron beam [12][13][14]28], and the other is to utilize space-field correlations in the undulator, such as by injecting a head-to-tail tilted beam into a transverse gradient undulator (TGU) [15] or a planar undulator [11]. Using a large energy-chirped electron beam is a simple and natural way to generate broadband XFEL radiation.…”
Section: Broadband Fel Pulse Generation In Sxfelmentioning
confidence: 99%
“…In addition to pursuing narrow-bandwidth FEL pulses, the large-bandwidth operation mode of XFEL has been proposed in recent years [11][12][13][14][15][16]. Because one broadband XFEL pulse covers the entire energy range of absorption spectra and the number of X-ray photons in each pulse reaches 10 12 , in principle, the XAS and XMCD experiments can be accomplished without major interactions with XFEL machine components.…”
Section: Introductionmentioning
confidence: 99%
“…where � r is the radiation wavelength, � u the undulator period, � the Lorentz factor of electrons and K the undulator parameter, there are basically two paths to generate large-bandwidth radiation with currently available undulators of fixed period. A possible method is to introduce a transverse tilt in the electron bunch passing through downstream undulators with considerable transverse variation of the undulator parameter like transverse gradient undulators (Prat et al, 2016) or natural gradient of planar undulators (Song et al, 2018). This kind of transversely tilted bunches can be achieved by radiofrequency (RF) deflecting cavity or corrugated structure.…”
Section: Introductionmentioning
confidence: 99%
“…According to the FEL resonance condition [21], the wavelength of FEL radiation is determined by the electron beam energy and the undulator field parameters. In principle, properly sending the head-tail tilted electron bunches into a transverse gradient undulator [22] or into a planar undulator with natural gradient [23] can make different parts of the bunch experience different magnetic field, and thus generate broadband FEL pulses. Besides that, using electron beams with time-energy correlation is a more natural way to obtain broad-bandwidth FEL, which may be achieved without additional hardware elements in currently existed facilities.…”
Section: Introductionmentioning
confidence: 99%