2022
DOI: 10.1088/1361-6641/ac45c0
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On the compact modelling of Si nanowire and Si nanosheet MOSFETs

Abstract: In this paper, 3D TCAD simulations are used to show that the electron concentration, current density, and electric field distribution from the interface at the lateral channels and from the top channel to the centre of the silicon wire, in Nanowire and Nanosheet structures, are practically same. This characteristic makes possible to consider that the total channel width for these structures is equal to the perimeter of the transistor sheet, allowing to extend the application of the Symmetric Doped Double-Gate … Show more

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Cited by 3 publications
(6 citation statements)
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“…For correcting the maximum mobility variation with temperature, expression (4) is applied 18 : μ0EFgoodbreak=μ0)(T300ξ,$$ {\mu}_{0\mathrm{EF}}=\frac{\mu_0}{{\left(\frac{T}{300}\right)}^{\xi }}, $$ where ξ is a thermal mobility factor used as an adjusting parameter.…”
Section: Analytical Models For the Drain And Gate Currents Of Nanowir...mentioning
confidence: 99%
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“…For correcting the maximum mobility variation with temperature, expression (4) is applied 18 : μ0EFgoodbreak=μ0)(T300ξ,$$ {\mu}_{0\mathrm{EF}}=\frac{\mu_0}{{\left(\frac{T}{300}\right)}^{\xi }}, $$ where ξ is a thermal mobility factor used as an adjusting parameter.…”
Section: Analytical Models For the Drain And Gate Currents Of Nanowir...mentioning
confidence: 99%
“…In references 17,18, an analytical model for the drain current ( I DS ) as a function of the applied voltages at the gate ( V GS ) and drain ( V DS ) terminals of nanowire MOS transistors has been proposed and validated at room temperature. In this model, the drain current is a function of the mobile charges at the source and drain ends of the channel ( q ns and q nd , respectively), normalized by C i kT/q , where Ci=εox/tox$$ {C}_{\mathrm{i}}={\varepsilon}_{\mathrm{ox}}/{t}_{\mathrm{ox}} $$ is the gate insulator capacitance per unit area, ε ox is the oxide permittivity, k is the Boltzmann constant, T is the absolute temperature, and q is the electron charge: IDSgoodbreak=2WLCi0.25emk0.25emTq0.25emμs1LL12)(qns2goodbreak−qnd2+2qnsqndqnormalblnqns+qbqnd+qbSN1+μsVDefvsatL20.5em][1goodbreak+2WLCi0.25emk0.25emTq0.25emR0.25emμs0.5em)(VGSgoodbreak−VTgoodbreak−CnormalSCS+CiVDef0.25em,$$ {I}_{\mathrm{DS}}=\frac{2\frac{W}{L}{C}_{\mathrm{i}}\ \frac{k\ T}{q}\ {\mu}_{\mathrm{s}}}{\left(1-\frac{\Delta L}{L}\right)}\frac{\frac{1}{2}\left({q}_{\mathrm{ns}}^2-{q}_{\mathrm{nd}}^2\right)+{\left[2\left({q}_{\mathrm{ns}}-{q}_{\mathrm{nd}}\right)-{q}_{\mathrm{b}}\ln \left(\frac{q_{\mathrm{ns}}+{q}_{\mathrm{b}}}{q_{\mathrm{nd...…”
Section: Analytical Models For the Drain And Gate Currents Of Nanowir...mentioning
confidence: 99%
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