The Atomic, Molecular and Optical Science instrument at the Linac Coherent Light Source

Ferguson, K.R.; Bucher, M.; Bozek, J.D.; Carron, S.; Castagna, J.-C.; Coffee, R.; Curiel, G.I.; Holmes, M.; Krzywinski, J.; Messerschmidt, M.; Minitti, M.; Mitra, A.; Moeller, S.; Noonan, P.; Osipov, T.; Schorb, S.; Swiggers, M.; Wallace, A.; Yin, J.; Bostedt, C.

doi:10.1107/S1600577515004646

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Figure 4
Stimulated Raman scattering setup at the AMO instrument. In (a) the XFEL beam is focused by the KB optics system into a high-pressure gas cell filled with neon. A grating spectrometer is used to separate the FEL and Raman signal. The Raman signal and FEL pulse in (b) are separated by approximately 20 eV. Figure reprinted with permission from Weninger et al. (2013

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 22| Part 3| May 2015| Pages 492-497

https://doi.org/10.1107/S1600577515004646

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