1991
DOI: 10.1016/0168-583x(91)95560-z
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Modeling charge collection and single event upsets in microelectronics

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Cited by 33 publications
(4 citation statements)
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“…(7) might then be replaced by a step function: oion(E)=o, for E%C. EC can be chosen [7,14] as the value for which ai011 rises to 50% of om. …”
Section: The Semi-empirical Modelmentioning
confidence: 99%
“…(7) might then be replaced by a step function: oion(E)=o, for E%C. EC can be chosen [7,14] as the value for which ai011 rises to 50% of om. …”
Section: The Semi-empirical Modelmentioning
confidence: 99%
“…While this prototype microdosimeter, with an array of micron size SVs, allowed acquisition of spectra related to gamma and neutrons interactions, quantification of microdosimetric spectra was impossible due to lack of well-defined sensitive volume geometry. Later, McNulty et al (1991) and Roth et al (1994) developed a silicon microdosimeter based on memory devices (993L422, 1 kByte). The system was intended for radiation monitoring in spacecraft and avionics.…”
Section: Solid-state Detectorsmentioning
confidence: 99%
“…Below the cylinders, the probability that a generated charge reaches cylinder i is proportional to the solid angle i subtended by the base of that cylinder. This can be seen as a first-level approximation based on the random-walk nature of the diffusion process [58]. If a charge reaches the cylinder base, it will be collected with the same efficiency as all charges inside the cylinder.…”
Section: Charge-collection Analysismentioning
confidence: 99%