2013
DOI: 10.1117/12.2018039
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High speed multichannel time-correlated single photon counting electronics based on SiGe integrated time-to-digital converters

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Cited by 3 publications
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“…The time correlation is provided by a PicoHarp 300 correlator (PicoQuant) triggered by a laser pulse. To avoid the pile-up effect, only 5% of the detected photon count was used to build the histograms …”
Section: Experimental Setup Descriptionmentioning
confidence: 99%
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“…The time correlation is provided by a PicoHarp 300 correlator (PicoQuant) triggered by a laser pulse. To avoid the pile-up effect, only 5% of the detected photon count was used to build the histograms …”
Section: Experimental Setup Descriptionmentioning
confidence: 99%
“…To avoid the pile-up effect, only 5% of the detected photon count was used to build the histograms. 17 …”
Section: Experimental Setup Descriptionmentioning
confidence: 99%
“…Being careful to account for dark count rates, taking care to avoid pile-up from prior excitation events, and implementing other best practices of PL decay measurement, some perovskite samples excited under low fluence do indeed show nearly textbook first-order decays. , However, many other samples show more complicated PL kinetics, even in the low-level injection regime. , As discussed in the SI section I, even in state-of-the-art perovskite compositions for photovoltaics, bimolecular recombination kinetics only become significant at CW excitation powers ∼a few mW/cm 2 (or fast pulsed fluences of >10 11 photons/pulse/cm 2 ) (Figures S1–S5, Tables S2–S4), and Auger rates only become significant at CW excitation powers exceeding ∼100 W/cm 2 (or fast pulsed fluences >10 14 photons/pulse/cm 2 ) . Thus, at lower powers/fluences we need to look to explanations other than higher-order kinetics to explain the observed non-single exponential carrier recombination dynamics.…”
mentioning
confidence: 99%