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Figure 8
Observed and simulated normalized integrated signal plotted as a function of the phase delay between the X-ray pulse and the beginning of integration, for a highly attenuated 29.2 keV beam. At the attenuation used, much of the signal was from X-ray energies of 58.4 keV and higher. These photons convert at a much greater depth in the sensor, causing the current pulse from the holes to be extended over a greater period of time (∼80 ns for 95% charge collection).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 31| Part 5| September 2024|
https://doi.org/10.1107/S160057752400643X
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