1988
DOI: 10.1109/5.4401
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Unified presentation of 1/f noise in electron devices: fundamental 1/f noise sources

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Cited by 275 publications
(89 citation statements)
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“…The dependence on the dark current, fitted quadratically in Fig. 3a, indicates that a-2, hinting to dominant volume trapping instead of a surface nature 37 . Regarding the impact on imaging, the high flicker noise for integration times in the range of 1 s is not detrimental as for most imaging applications integrations times are in the millisecond range.…”
Section: Resultsmentioning
confidence: 99%
“…The dependence on the dark current, fitted quadratically in Fig. 3a, indicates that a-2, hinting to dominant volume trapping instead of a surface nature 37 . Regarding the impact on imaging, the high flicker noise for integration times in the range of 1 s is not detrimental as for most imaging applications integrations times are in the millisecond range.…”
Section: Resultsmentioning
confidence: 99%
“…Although other physical mechanisms of LFN may co-exist [109,116,117], interface traps are usually employed to understand the origin of LFN in graphene devices [61,65,102,118,119]. For instance, suspended graphene devices show a 6-12 times lower LFN than those with a SiO 2 substrate, suggesting that the traps in SiO 2 substrate contribute significantly to LFN [118].…”
Section: B Device Fluctuations From Many Interface Trapsmentioning
confidence: 99%
“…The McWhorter model views the LFN as the multi-level fluctuations caused by an ensemble of many interface traps (number >>1): each trap contributes a RTN over a wide range of  and corner f (see Figure 2a) [109,117,120,121]. The overall PSD can be integrated as [65].…”
Section: B Device Fluctuations From Many Interface Trapsmentioning
confidence: 99%
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