Paper | Title | Page |
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WEA1IO01 |
Demonstration of Energy-Chirp Control in Relativistic Electron Bunches at LCLS Using a Corrugated Structure | |
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An experimental study is presented of a corrugated structure that uses wakefields to remove linear energy correlation in a high energy (4.4 - 13.3 GeV) electron beam (a dechirper). Time-resolved measurements of both longitudinal and transverse wakefields of the device are presented and compared with simulations. We demonstrate flexible control of the LCLS FEL bandwidth and present novel uses of the device in addition to energy chirp control. | ||
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Slides WEA1IO01 [18.218 MB] | |
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WEPOB30 | Simulation of the Shot-Noise Driven Microbunching Instability Experiment at the LCLS | 967 |
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The shot-noise driven microbunching instability can significantly degrade electron beam quality in next generation light sources. Experiments were carried out at the Linac Coherent Light Source (LCLS) to study this instability. In this paper, we will present start-to-end simulation of the shot-noise driven microbunching instability experiment at the LCLS. | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-WEPOB30 | |
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WEPOB49 | LCLS Injector Laser Profile Shaping Using Digital Micromirror Device | 1001 |
SUPO22 | use link to see paper's listing under its alternate paper code | |
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In the Linear Coherent Light Source (LCLS) at SLAC, the injector laser plays an important role as the source of the electron beam for the Free Electron Laser (FEL). The emittance of the beam is highly related to the transverse profile of the injector laser. Currently the LCLS injector laser has undesired features, such as hot spots, which carry over to the electron beam. These undesired features increase electron emittance, degrade the FEL performance, and complicate operations. The injector laser shaping project at LCLS aims to produce arbitrary electron beam profiles, such as cut-Gaussian, uniform, and parabolic, and to study the effect of spatial profiles on beam emittance and FEL performance. Effectively it also allows easy transition between the two spare lasers, where the operators can use the spatial shaper to achieve identical profiles for the two lasers. In this paper, we describe the experimental methods to achieve laser profile shaping and electron beam profile shaping respectively, and demonstrate promising results. | ||
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Poster WEPOB49 [1.850 MB] | |
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-WEPOB49 | |
Export • | reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml) | |