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 5
Horizontal e-beam profiles measured at WS3 (a), the third scanner in Fig. 4

, and WS5 (b), the fifth scanner, before and after the lattice matching. The distance marked in the figure represents the peak position shift of the electron beam distribution after the matching, while the position of center of mass appears unchanged after the matching.

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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