1986
DOI: 10.1016/0038-1101(86)90078-x
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On the current transport mechanism in a metal—insulator—semiconductor (MIS) diode

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Cited by 197 publications
(85 citation statements)
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“…This kind of MIS stack has been studied theoretically and experimentally with a precise control over the growth process and layer thicknesses in the past (36)(37)(38)(39)(40)(41)(42)(43). However, the numerical values calculated for different parameters in previous studies cannot be directly used for modeling and comparison here, because our device has a much different structure that includes particles with random shapes, oxide layers with inhomogeneous properties and the organic binder.…”
Section: Resultsmentioning
confidence: 99%
“…This kind of MIS stack has been studied theoretically and experimentally with a precise control over the growth process and layer thicknesses in the past (36)(37)(38)(39)(40)(41)(42)(43). However, the numerical values calculated for different parameters in previous studies cannot be directly used for modeling and comparison here, because our device has a much different structure that includes particles with random shapes, oxide layers with inhomogeneous properties and the organic binder.…”
Section: Resultsmentioning
confidence: 99%
“…where A is the area of diode, N d is the doping concentration, V d is the diffusion potential at zero bias [24]. The depletion layer width can be expressed as…”
Section: Resultsmentioning
confidence: 99%
“…The operation frequency is 100 kHz and the voltage is swept from 0 V to 4 V under reverse bias of the diode. The relationship between depletion capacitance C and the applied voltage can be expressed as [15,16]:…”
Section: Resultsmentioning
confidence: 99%