view article

Figure 1
Illustration of a deconvolution approach using a realistic X-ray pulse profile. (a) The X-ray pulse profile used for these simulations, which approximates the measured single-bunch pulse profile of the ESRF (courtesy of K. Scheidt and G. Naylor). (b) A comparison between the measurement of an exponential decay, [\Delta I(t)\propto\exp(-t/\tau)], after deconvolution (solid line) with an idealized measurement (dashed line). Experimental noise was taken to obey a Gaussian distribution with standard deviation [\sigma] = 5% of [\Delta I]max, 100 steps of [\Delta t] = 18 ps were taken, and the deconvoluted signal was numerically filtered. (c) A comparison between two further simulations with the decay constant [\tau] = 30 ps, where 100 steps of [\Delta t] = 12 ps were taken. Deconvoluted intensities as a function of time, in combination with a spectroscopic characterization of the time scales of interest, would provide a starting point from which to build and refine the sample's rapid structural dynamics. Intensity units are arbitrary.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Follow J. Synchrotron Rad.
Sign up for e-alerts
Follow J. Synchrotron Rad. on Twitter
Follow us on facebook
Sign up for RSS feeds