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 6
Left: the pulse train difference, ΔS_PT(q, p), calculated from the laser off measurements of a pump–probe scan. Middle: the best fit to ΔS_PT of the model defined by equation (5)

. Right: the residual of the model fit. These data were measured during experiment A.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

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

https://doi.org/10.1107/S1600577525009737

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