Analysis strategies for time-resolved X-ray solution scattering at high repetition rate XFEL sources

Haubro, M.L.; Zederkof, D.B.; Khakhulin, D.; Yousef, H.; Jiang, Y.; Macias, I.J.B.; Kluyver, T.; Lima, F.; Biednov, M.; Milne, C.; Uemura, Y.; Zalden, P.; Wang, H.; Dohn, A.O.; Mitterer, K.; Markmann, V.; Ohlson, O.; Wachter-Lehn, M.T.; Lenzen, P.; Jensen, B.K.; Høholdt, A.; van Driel, T.B.; Nimmrich, A.; Selenius, E.; Levi, G.; Møller, K.B.; Nielsen, M.M.; Haldrup, K.

doi:10.1107/S1600577525009737

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Figure 7
The scattering components contributing to the fitted model. Left: ΔS_ΔT and ΔS_Δρ from Kjaer et al. (2013

), scaled by the number of water molecules in the LUC (2750). Right: $[S_{{\rm H_{2}O,liq}}]$ , the scattering signal from liquid water scaled to one water molecule (Skinner et al., 2013

), and $[S_{{\rm H_{2}O,gas}}]$ , the X-ray scattering calculated for a single gaseous water molecule. Both scattering signals also include Compton scattering.

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Volume 33| Part 1| January 2026| Pages 18-31

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