Rapid sample delivery for megahertz serial crystallography at X-ray FELs

Wiedorn, M.O.; Awel, S.; Morgan, A.J.; Ayyer, K.; Gevorkov, Y.; Fleckenstein, H.; Roth, N.; Adriano, L.; Bean, R.; Beyerlein, K.R.; Chen, J.; Coe, J.; Cruz-Mazo, F.; Ekeberg, T.; Graceffa, R.; Heymann, M.; Horke, D.A.; Knoška, J.; Mariani, V.; Nazari, R.; Oberthür, D.; Samanta, A.K.; Sierra, R.G.; Stan, C.A.; Yefanov, O.; Rompotis, D.; Correa, J.; Erk, B.; Treusch, R.; Schulz, J.; Hogue, B.G.; Gañán-Calvo, A.M.; Fromme, P.; Küpper, J.; Rode, A.V.; Bajt, S.; Kirian, R.A.; Chapman, H.N.

doi:10.1107/S2052252518008369

Figure 5
Sideview images showing the arrival of the second X-ray pulse in a train of pulses. The water jet was operated under the same conditions described in Fig. 4

. The horizontal red line indicates that the jet has recovered and is stable in the X-ray interaction region after <290 ns. The last image in the sequence shows the jet after being hit by the second pulse in the pulse train. The scale bar is 20 µm. X-rays are incident from the left.

IUCrJ

Volume 5| Part 5| September 2018| Pages 574-584

ISSN: 2052-2525

https://doi.org/10.1107/S2052252518008369

PHYSICS | FELS

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