2020
DOI: 10.1109/tns.2020.2998433
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A Photomultiplier With an AlGaN Photocathode and Microchannel Plates for BaF2 Scintillator Detectors in Particle Physics

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Cited by 6 publications
(2 citation statements)
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“…A high fraction of the slow component (about 85%) in the total luminescence can cause pile-up of signals at a high beam rate. To solve this problem, various approaches are being investigated: 1) the use of thin films on an avalanche photodetector [7] to suppress luminescence above 280 nm, 2) the use of a thin multilayer filter on the quartz glass substrate between the crystal and the photodetector to suppress luminescence in the range 250-400 nm [8], 3) the use of a solar-blind photomultiplier with an aluminum-gallium nitride (AlGaN) photocathode [9], 4) suppression of the slow scintillation component by doping a BaF 2 crystal with yttrium [10].…”
Section: Introductionmentioning
confidence: 99%
“…A high fraction of the slow component (about 85%) in the total luminescence can cause pile-up of signals at a high beam rate. To solve this problem, various approaches are being investigated: 1) the use of thin films on an avalanche photodetector [7] to suppress luminescence above 280 nm, 2) the use of a thin multilayer filter on the quartz glass substrate between the crystal and the photodetector to suppress luminescence in the range 250-400 nm [8], 3) the use of a solar-blind photomultiplier with an aluminum-gallium nitride (AlGaN) photocathode [9], 4) suppression of the slow scintillation component by doping a BaF 2 crystal with yttrium [10].…”
Section: Introductionmentioning
confidence: 99%
“…However, a high fraction of the slow component (about 85%) in the total luminescence can cause pile-up of signals at a high beam rate. To solve this problem, various approaches are being investigated: 1) the use of thin films on an avalanche photodetector [6] to suppress luminescence above 280 nm, 2) the use of a thin multilayer filter on the quartz glass substrate between the crystal and the photodetector to suppress luminescence in the range 250-400 nm [7], 3) the use of a solar-blind photomultiplier with an aluminum-gallium nitride (AlGaN) photocathode [8], 4) suppression of the slow scintillation component by doping a BaF 2 crystal with yttrium [9].…”
Section: Introductionmentioning
confidence: 99%