2014
DOI: 10.1016/j.microrel.2014.01.024
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Modelling RTN and BTI in nanoscale MOSFETs from device to circuit: A review

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Cited by 38 publications
(15 citation statements)
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“…With the experimentally determined g0, m, n, and η as the inputs, µ_ ΔVthGD and µ_ NGD at any Vgov and t can be calculated by eqs. (1) and (5), respectively. If one uses M devices for each stress time, the number of traps per device can be randomly assigned using the Poisson distribution of an average µ_NGD and the impact of each trap on a device, δVthGD, can be generated from the exponential distribution.…”
Section: A Within-device-fluctuation (Wdf) Of Gdsmentioning
confidence: 99%
See 1 more Smart Citation
“…With the experimentally determined g0, m, n, and η as the inputs, µ_ ΔVthGD and µ_ NGD at any Vgov and t can be calculated by eqs. (1) and (5), respectively. If one uses M devices for each stress time, the number of traps per device can be randomly assigned using the Poisson distribution of an average µ_NGD and the impact of each trap on a device, δVthGD, can be generated from the exponential distribution.…”
Section: A Within-device-fluctuation (Wdf) Of Gdsmentioning
confidence: 99%
“…As the CMOS nodes scale down to nano-meter regime, time-dependent variations induced by negative bias temperature instability (NBTI) has become a big concern for circuit design [1][2][3][4][5]. These nano-scaled devices are dominated by only a handful of defects, which are usually categorized into the recoverable and permanent components [6].…”
Section: Introductionmentioning
confidence: 99%
“…Another important reliability issue in miniaturized devices is the so called bias temperature instabilities (BTI) [ 19 , 20 , 21 , 22 , 23 , 24 ]. BTI typically manifest as a drift of the drain-source current over time when constant biases are applied to a transistor, and is studied up electric oxide fields of .…”
Section: Introductionmentioning
confidence: 99%
“…In one test device, two active traps (D1 and D2) can be identified during the monitoring step measurement in the pristine state, as is apparent from the two distinct|Id| recovery steps in some of the selected relaxation traces (Figure 4 trapping by the CHH stress [137], as is manifested by the upshift in |Id| eoc after each stress. Simulation study [123] has shown that a trap's |Id| recovery step is dependent on the local inversion charge density, which is reduced after the generation of more positive oxide/interface trapped charges by the CHH stress.…”
Section: Channel Hot-hole Effectmentioning
confidence: 99%