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Figure 3
The accumulated Bragg signal I(t) = [({{1}/{T}})\,\,I_{0}\int^{t}_{0}\,k(q,t')\,h(q,t')\,s(t')\,\,{\rm{d}}t^{\,\prime}\,] as a function of time, from carbon at q = 0.62 Å−1. A 700 nm PSI crystal exposed to a 100 fs-long pulse at 6 keV and intensity 2 × 106 J cm−2 was simulated. The accumulated intensity I(t) is shown in J cm−2 and can be interpreted as an `effective' photon intensity that includes pulse shape and damage effects, and should be multiplied by the term [r_{\rm{e}}^{\,2}\Delta\Omega|F_{0}({\bf{q}})|^2].

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 22| Part 2| February 2015| Pages 256-266
doi:10.1107/S1600577515002878
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