Proceedings of 36th International Cosmic Ray Conference — PoS(ICRC2019) 2019
DOI: 10.22323/1.358.0834
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Sensitivity Improvements of Very-High-Energy $\gamma$-Ray Detection with the Upgraded H.E.S.S. I Cameras using Full Waveform Processing

Abstract: Peak time (ns) CM integration time Charge SMMax9 (a.u.) Figure 1: Cherenkov images (raw data charge and peak time) are shown, taken in SM and using a fixed 9 ns-wide integration window around the peak maximum of each signal for charge extraction (referred to as SMMax9, cf. Sec. 3 for more details). Additionally, the corresponding uncalibrated (raw data) waveforms of a few pixels are displayed and the part of the signal (first 16 ns) being integrated in CM is indicated.

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“…This mode is only used for selected targets, due to the much greater amount of data created when it is active. Initial results on the performance of this readout mode are reported in [30].…”
Section: Readout and Slow Controlmentioning
confidence: 99%
“…This mode is only used for selected targets, due to the much greater amount of data created when it is active. Initial results on the performance of this readout mode are reported in [30].…”
Section: Readout and Slow Controlmentioning
confidence: 99%