2015
DOI: 10.1118/1.4931979
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Systematic evaluation of photodetector performance for plastic scintillation dosimetry

Abstract: For dose rates higher than 3 mGy/s, the PIN diode is the most effective photodetector in terms of performance/cost ratio. For lower dose rates, such as those seen in interventional radiology or high-gradient radiotherapy, PMTs are the optimal choice.

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Cited by 19 publications
(24 citation statements)
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“…In those conditions, precise measurements can be made by either short (about 2 s) or long (.30 s) exposure times. These conclusions are in agreement with Boivin et al 31 recommendations concerning the dose rate ranges of use for one-dimensional plastic scintillation detector with a PIN diode photodetector.…”
Section: Linearitysupporting
confidence: 81%
“…In those conditions, precise measurements can be made by either short (about 2 s) or long (.30 s) exposure times. These conclusions are in agreement with Boivin et al 31 recommendations concerning the dose rate ranges of use for one-dimensional plastic scintillation detector with a PIN diode photodetector.…”
Section: Linearitysupporting
confidence: 81%
“…When developing ISDs based on Eu-activated phosphors, the scintillation intensity should be maximized by optimizing the phosphor-glue ratio to limit the influence of stem signal contamination and to minimize the statistical uncertainty of time-resolved measurements. In addition to shortening the fiber-optic cable to about 2 m, choosing a more sensitive photodetector than the one we used could further minimize the statistical uncertainty (Boivin et al 2015). …”
Section: Discussionmentioning
confidence: 99%
“…PMTs were chosen as the photodetectors because they have a high signal to noise ratio (SNR) and readout speed that overcomes many of the sensitivity issues of charge‐coupled device‐based systems. Generally, PMTs more accurately measure low light signals and have a faster response, making them more suitable for the demands of in vivo dosimetry applications . Henceforth, an assembly composed of a dichroic mirror, filter, and PMT will be referred to as a “channel.” From an optimization perspective, the signal produced in each channel was calculated, taking into account the measured scintillation spectrum and light yield, the manufacturer‐reported transmission and attenuation of the optical components, and the experimentally characterized PMT noise.…”
Section: Methodsmentioning
confidence: 99%