2006
DOI: 10.1134/s1063782606090193
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Spectrometric properties of SiC detectors based on ion-implanted p +-n junctions

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Cited by 8 publications
(11 citation statements)
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“…It could be used to interpret the difference of trigger efficiency for 5mm×5mm (4.7 events/min) and 1.5mm×1.5mm (2.1 events/min) size 4H-SiC-PIN where large size has higher trigger efficiency. The MPV of energy deposition in 100 µm 4H-SiC layer is 55 MeV which is a little higher than the previous experimental result (∼42 MeV) [10] due to scattering effects by aluminum foil and LGAD as well as the ionization track is longer than 100 µm.…”
Section: Energy Response By Geant4 Simulationcontrasting
confidence: 65%
“…It could be used to interpret the difference of trigger efficiency for 5mm×5mm (4.7 events/min) and 1.5mm×1.5mm (2.1 events/min) size 4H-SiC-PIN where large size has higher trigger efficiency. The MPV of energy deposition in 100 µm 4H-SiC layer is 55 MeV which is a little higher than the previous experimental result (∼42 MeV) [10] due to scattering effects by aluminum foil and LGAD as well as the ionization track is longer than 100 µm.…”
Section: Energy Response By Geant4 Simulationcontrasting
confidence: 65%
“…The most probable values (MPVs) of the energy deposition in 100 μm 4H-SiC layer are 25 and 55 MeV for the two different energy β particles from the 90 Sr source. There are little differences with the previous experimental result (~42 MeV)[25] due to scattering effects by the aluminum foil and LGAD, which make the ionization track slightly longer than 100 μm, but the average MPV of energy deposition from these two particles is close to the experimental result.TIME RESOLUTION OF 4H-SIC PIN Waveform SamplingThe two channels are triggered at the same time with different trigger levels for waveform sampling. Trigger Ref = 25 mV and trigger DUT = 15 mV are determined by noise levels (see Figure7) to suppress noise spikes.…”
supporting
confidence: 61%
“…The structures with such p + -n junctions were characterized by a differential resistance of ≤ 3 × 10 -3 Ω m -2 in the forward direction and by a breakdown voltage of 1700 V. The current in a reversely biased structure exhibited a linear growth with the temperature up to 400 ° C. This was evidence of the absence of microplasma breakdowns and peripheral leakage currents in the detector structures in the entire temperature interval studied. This behavior also indicated that a low level of detector noise could be expected at elevated temperatures [5].…”
Section: Introduction Wide-bandgap Semiconductorsmentioning
confidence: 80%
“…Such an emitter can serve as an effective entrance window ensuring low energy losses. Indeed, 4H-SiC detectors with ion-doped p + -n junctions exhibited a 100% CCE for α -particle-generated charge with an energy resolution of ≤ 2% [5]. Using such structures, we have previously studied for the first time the spectrometric characteristics of detectors and four-detector arrays operating at a temperature of 170 ° C and 140 ° C, respectively [6,7].…”
Section: Introduction Wide-bandgap Semiconductorsmentioning
confidence: 99%
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