2013
DOI: 10.1109/ted.2013.2287528
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A Common Core Model for Junctionless Nanowires and Symmetric Double-Gate FETs

Abstract: In this paper, we evidence the link between the planar and cylindrical junctionless field effect transistors (JL-FETs) from the electrostatics and current point of view. In particular, we show that an approximate solution of the Poisson-Boltzmann equation for JL nanowires can be mapped on the planar doublegate topology generating only negligible mismatch, meaning that both devices can share the same core model as far as long channels are considered. These preliminary results are a first step toward a unificati… Show more

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Cited by 49 publications
(16 citation statements)
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“…These noise models represent the first step toward compact modeling of thermal noise in JL FETs devices. In addition, based on the equivalence between planar and cylindrical JL FETs [10], we expect that such a model could also be appropriate for JL NW.…”
Section: Discussionmentioning
confidence: 99%
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“…These noise models represent the first step toward compact modeling of thermal noise in JL FETs devices. In addition, based on the equivalence between planar and cylindrical JL FETs [10], we expect that such a model could also be appropriate for JL NW.…”
Section: Discussionmentioning
confidence: 99%
“…Note that when the whole channel operates in depletion, Y FB = 0 is imposed in (7)- (10). Similarly, when the whole channel is in accumulation, Y FB = L G holds in (3)-(6).…”
Section: B Spatial Dependence Of the Mobile Charge Densitymentioning
confidence: 99%
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“…To understand this different conduction mechanism analytically, several models have been introduced for double-gate junctionless transistors (DGJL-FETs). Current-voltage models have been introduced [6], [7] and analytical threshold voltage models have been developed [8]- [10] for symmetric DGJL-FETs. However, a general potential model represented with analytic formulas for tied and untied DGJL-FETs with corresponding symmetric and asymmetric structures has not yet been developed.…”
Section: Introductionmentioning
confidence: 99%
“…Device simulations are conducted with the aid of the SILVACO 2-D simulator using the Lombardi mobility model along with Shockley-Read-Hall and Fermi-Dirac carrier statistics [13]. We neglect quantum mechanical effects because the simulated channel is thicker than 10 nm in the doping concentration of 1 × 10 19 cm −3 or less [7], [8]. In addition, we also ignore the parasitic series resistance arisen from the S/D extension in order to simplify the model.…”
Section: Introductionmentioning
confidence: 99%