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Figure 5
Signal (integrated current) measured for the current pulses shown in Fig. 2[link] as a function of the phase delay between the induced current pulse and a 300 ns-long charge integration window. The length of the window is chosen to be longer than the length of the current pulse. The curves are normalized to the total charge contained in the pulse. These curves directly show the total fraction of charge that can be collected within a given time window. The rising and falling edges contain equivalent information about the charge collection dynamics. We have chosen to show the falling edge (as highlighted by the gray box) in Figs. 6[link] and 7[link] since the ASIC amplifier is known to be faster on the falling edge.

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