2011
DOI: 10.1103/physrevstab.14.090701
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Measurement of the average local energy spread of electron beam via coherent harmonic generation

Abstract: The local energy spread of electron beam is a very important parameter for high-gain free-electron lasers (FELs), especially the seeded FELs. Highly accurate measurement of the extremely small local energy spread is rather challenging. In this paper, a simple method to accurately measure the average local energy spread based on the coherent harmonic generation is proposed. A one-dimensional analytical estimation is given to show the principle of this method, and three-dimensional simulation codes have been use… Show more

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Cited by 29 publications
(18 citation statements)
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“…The microbunched electron beam is then sent through the crossed-planar radiators, which are tuned to be resonant at the second harmonic of the seed laser, to produce coherent FEL radiation at the central wavelength of 523 nm. Using the modified optical replica method [36][37], critical parameters for the density modulation, such as the sliced beam energy spread and the energy modulation amplitude induced by the seed laser, were precisely quantified. In this experiment, the sliced beam energy spread and the energy modulation amplitude were measured to be 1.2 and 12 keV, respectively, which corresponds to a strong bunching factor over 40% for 523 nm radiation at the entrance of the radiators.…”
mentioning
confidence: 99%
“…The microbunched electron beam is then sent through the crossed-planar radiators, which are tuned to be resonant at the second harmonic of the seed laser, to produce coherent FEL radiation at the central wavelength of 523 nm. Using the modified optical replica method [36][37], critical parameters for the density modulation, such as the sliced beam energy spread and the energy modulation amplitude induced by the seed laser, were precisely quantified. In this experiment, the sliced beam energy spread and the energy modulation amplitude were measured to be 1.2 and 12 keV, respectively, which corresponds to a strong bunching factor over 40% for 523 nm radiation at the entrance of the radiators.…”
mentioning
confidence: 99%
“…Thus, CHG intensity is much higher than spontaneous emission even at the very beginning of the radiator. The intensity analysis of such coherent photon beam can be used to roughly estimate the temporal structure of the electron beam current and emittance [36], or precisely determine the averaged slice energy spread [37,38], while spatial profile studies, as we will show below, will allow one to optimize the electron beam trajectory, verify the undulator magnetic gap, and adjust the phase match between two undulator segments.…”
Section: Coherent Photon Beam Based Methodsmentioning
confidence: 99%
“…A large bunching factor at high harmonics relies on the formation of sharp density spikes, which requires large energy modulation amplitude. For an HGHG FEL, the energy modulation amplitude A should be n times larger than the initial energy spread to give a considerable value of bunching factor at nth harmonic [25,26]. However, as shown in Fig.…”
Section: Hghg and Eehg With Short Seed Pulsesmentioning
confidence: 99%