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Gallium Nitride Room Temperature α Particle Detectors 被引量:3

Gallium Nitride Room Temperature α Particle Detectors
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摘要 Gallium Nitride (GaN) room temperature α particle detectors are fabricated and characterized, whose device structure is Schottky diode. The current-voltage (I- V) measurements reveal that the reverse breakdown voltage of the detectors is more than 200 V owing to the consummate fabrication processes, and that the Schottky barrier and ideal factor of the detectors are 0.64 eV and 1.02, respectively, calculated from the thermionic transmission model. ^241Am α particles pulse height spectra from the GaN detectors biased at -8 V is obviously one Gauss peak located at channel 44 with the full width at half maximum (FWHM) of 15.87 in channel. One of the main reasons for the relatively wider FWHM is that the air between the detectors and isotope could widen the spectrum. Gallium Nitride (GaN) room temperature α particle detectors are fabricated and characterized, whose device structure is Schottky diode. The current-voltage (I- V) measurements reveal that the reverse breakdown voltage of the detectors is more than 200 V owing to the consummate fabrication processes, and that the Schottky barrier and ideal factor of the detectors are 0.64 eV and 1.02, respectively, calculated from the thermionic transmission model. ^241Am α particles pulse height spectra from the GaN detectors biased at -8 V is obviously one Gauss peak located at channel 44 with the full width at half maximum (FWHM) of 15.87 in channel. One of the main reasons for the relatively wider FWHM is that the air between the detectors and isotope could widen the spectrum.
出处 《Chinese Physics Letters》 SCIE CAS CSCD 2010年第5期69-71,共3页 中国物理快报(英文版)
基金 Supported by the National Natural Science Foundation of China under Grant No 10875084, the Natural Science Foundation of Jiangsu Province under Grant No BK2008174, the Applied Science Foundation of Suzhou under Grant No SYJG0915, and the National Basic Research Program of China under Grant No G2009CB929300.
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