The Macromolecular Femtosecond Crystallography Instrument at the Linac Coherent Light Source

Sierra, R.G.; Batyuk, A.; Sun, Z.; Aquila, A.; Hunter, M.S.; Lane, T.J.; Liang, M.; Yoon, C.H.; Alonso-Mori, R.; Armenta, R.; Castagna, J.-C.; Hollenbeck, M.; Osier, T.O.; Hayes, M.; Aldrich, J.; Curtis, R.; Koglin, J.E.; Rendahl, T.; Rodriguez, E.; Carbajo, S.; Guillet, S.; Paul, R.; Hart, P.; Nakahara, K.; Carini, G.; DeMirci, H.; Dao, E.H.; Hayes, B.M.; Rao, Y.P.; Chollet, M.; Feng, Y.; Fuller, F.D.; Kupitz, C.; Sato, T.; Seaberg, M.H.; Song, S.; van Driel, T.B.; Yavas, H.; Zhu, D.; Cohen, A.E.; Wakatsuki, S.; Boutet, S.

doi:10.1107/S1600577519001577

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Figure 7
Efficiency at 7.5 keV with no pre-focusing and pre-focusing using a lens of 750 µm radius (bottom stack), the only usable pre-focusing option at 7.5 keV. Pre-focusing increases the transmission by a factor of ∼2.5. The relative single-pulse intensity measured after the focusing optics is shown as dots versus the gas detector single pulse signal, with a linear fit as a line. The slope represents the relative efficiency.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 26| Part 2| March 2019| Pages 346-357

https://doi.org/10.1107/S1600577519001577

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