1967
DOI: 10.1109/tns.1967.4324452
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Afterpulses in Photomultipliers

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Cited by 71 publications
(27 citation statements)
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“…Even with a higher threshold, a single photoelectron event can result in a much larger "afterpulse" in the PMT [41,42]. This afterpulse results from contamination of the PMT vacuum over time (especially by helium, which diffuses through glass) and occurs between 400 ns and 600 ns after the initial pulse.…”
Section: Resultsmentioning
confidence: 99%
“…Even with a higher threshold, a single photoelectron event can result in a much larger "afterpulse" in the PMT [41,42]. This afterpulse results from contamination of the PMT vacuum over time (especially by helium, which diffuses through glass) and occurs between 400 ns and 600 ns after the initial pulse.…”
Section: Resultsmentioning
confidence: 99%
“…PMT afterpulses are parasitic signals composed of single or few photoelectrons, following a true scintillation event. They originate in residual gas atoms or molecules within the PMT, backflowing towards the photocathode or dynodes after their ionization by the electronic cascade from the primary event [106][107][108][109][110]. The bulk majority of PMT afterpulses appear a maximum of ∼15 µs after the primary, and hence the conservative length for this pretrace (specifically for the ET9390KB, this maximum delay has been reported to be ∼3 µs [111]).…”
Section: Methodsmentioning
confidence: 99%
“…1) PMT Afterpulsing: Exploration into the chemical and physical nature of PMT afterpulsing effects [33]- [35] showed that diffusion of trace gases through the tube envelope contributed to an increase in the probability of pulse formation. In particular, diffused helium was found to be the main source of afterpulses in tubes that are more than two years old.…”
Section: Causes Of Image Ghostingmentioning
confidence: 99%