FEL performance achieved at PAL-XFEL using a three-chicane bunch compression scheme

Kang, H.-S.; Yang, H.; Kim, G.; Heo, H.; Nam, I.; Min, C.-K.; Kim, C.; Baek, S.Y.; Choi, H.-J.; Mun, G.; Park, B.R.; Suh, Y.J.; Shin, D.C.; Hu, J.; Hong, J.; Jung, S.; Kim, S.-H.; Kim, K.; Na, D.; Park, S.S.; Park, Y.J.; Han, J.-H.; Jung, Y.G.; Jeong, S.H.; Kim, M.J.; Lee, H.G.; Lee, S.; Lee, W.-W.; Oh, B.; Suh, H.S.; Park, K.-H.; Lee, H.-S.; Khan, D.Z.; Raubenheimer, T.O.; Wu, J.

doi:10.1107/S1600577519005861

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Figure 1
Schematic diagram of PAL-XFEL. L0: injector; L1, L2, L3A, L3B, L4 and L3S: acceleration sections; X: X-band linearizer cavity; DF1, DF2H and DF2S: deflector cavities; LH: laser heater; BC1, BC2, BC3H and BC3S: magnetic bunch compressor chicanes, whose dipoles are rectangles in blue; BAS0, BAS1, BAS3H and BAS3S: beam analysis stations, each of which consists of a dipole (rectangle in blue), a YAG screen and a dump (rectangle in black).

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 26| Part 4| July 2019| Pages 1127-1138

https://doi.org/10.1107/S1600577519005861

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