Surface-Roughness-Induced Variability in Nanowire InAs Tunnel FETs

We present a comparative study of the surfaceroughness (SR)-induced variability at low supply voltage V DD = 0.3 V in nanowire InAs tunnel FETs and strained-silicon (sSi) MOSFETs. By exploiting a 3-D full-quantum approach based on the Non-Equilibrium Green's Function formalism, we show that the...

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Published inIEEE electron device letters Vol. 33; no. 6; pp. 806 - 808
Main Authors Conzatti, F., Pala, M. G., Esseni, D.
Format Journal Article
LanguageEnglish
Published New York, NY IEEE 01.06.2012
Institute of Electrical and Electronics Engineers
The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
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Abstract We present a comparative study of the surfaceroughness (SR)-induced variability at low supply voltage V DD = 0.3 V in nanowire InAs tunnel FETs and strained-silicon (sSi) MOSFETs. By exploiting a 3-D full-quantum approach based on the Non-Equilibrium Green's Function formalism, we show that the I on variability in InAs tunnel FETs is much smaller than the I off variability, whereas for V DD = 0.3 V, the sSi MOSFETs working in the subthreshold regime present similar I on and I off variability. We explain the smaller Ion compared with Ioff variability of InAs tunnel FETs by noting that in the source depletion region, where tunneling mainly occurs for V GS = V DD , microscopic subband fluctuations induced by SR are small compared to macroscopic band bending due to the built-in potential of the source junction and to the gate bias. This results in SR-induced variability that is larger in InAs tunnel FETs than in sSi MOSFETs.
AbstractList We present a comparative study of the surface-roughness (SR)-induced variability at low supply voltage [Formula Omitted] in nanowire InAs tunnel FETs and strained-silicon (sSi) MOSFETs. By exploiting a 3-D full-quantum approach based on the Non-Equilibrium Green's Function formalism, we show that the [Formula Omitted] variability in InAs tunnel FETs is much smaller than the [Formula Omitted] variability, whereas for [Formula Omitted], the sSi MOSFETs working in the subthreshold regime present similar [Formula Omitted] and [Formula Omitted] variability. We explain the smaller [Formula Omitted] compared with [Formula Omitted] variability of InAs tunnel FETs by noting that in the source depletion region, where tunneling mainly occurs for [Formula Omitted], microscopic subband fluctuations induced by SR are small compared to macroscopic band bending due to the built-in potential of the source junction and to the gate bias. This results in SR-induced variability that is larger in InAs tunnel FETs than in sSi MOSFETs.
We present a comparative study of the surface-roughness (SR)-induced variability at low supply voltage ... in nanowire InAs tunnel FETs and strained-silicon (sSi) MOSFETs. By exploiting a 3-D full-quantum approach based on the Non-Equilibrium Green's Function formalism, we show that the ... variability in InAs tunnel FETs is much smaller than the ... variability, whereas for ..., the sSi MOSFETs working in the subthreshold regime present similar ... and ... variability. We explain the smaller ... compared with ... variability of InAs tunnel FETs by noting that in the source depletion region, where tunneling mainly occurs for ..., microscopic subband fluctuations induced by SR are small compared to macroscopic band bending due to the built-in potential of the source junction and to the gate bias. This results in SR-induced variability that is larger in InAs tunnel FETs than in sSi MOSFETs.
We present a comparative study of the surfaceroughness (SR)-induced variability at low supply voltage V DD = 0.3 V in nanowire InAs tunnel FETs and strained-silicon (sSi) MOSFETs. By exploiting a 3-D full-quantum approach based on the Non-Equilibrium Green's Function formalism, we show that the I on variability in InAs tunnel FETs is much smaller than the I off variability, whereas for V DD = 0.3 V, the sSi MOSFETs working in the subthreshold regime present similar I on and I off variability. We explain the smaller Ion compared with Ioff variability of InAs tunnel FETs by noting that in the source depletion region, where tunneling mainly occurs for V GS = V DD , microscopic subband fluctuations induced by SR are small compared to macroscopic band bending due to the built-in potential of the source junction and to the gate bias. This results in SR-induced variability that is larger in InAs tunnel FETs than in sSi MOSFETs.
Author Pala, M. G.
Conzatti, F.
Esseni, D.
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Issue 6
Keywords MOS technology
MOSFET
Band bending
Tunnel effect
Roughness
Subband
variability
Green function
tunnel-FET
surface roughness
Field effect transistor
Low voltage
Nanowire device
Non equilibrium conditions
Silicon
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Snippet We present a comparative study of the surfaceroughness (SR)-induced variability at low supply voltage V DD = 0.3 V in nanowire InAs tunnel FETs and...
We present a comparative study of the surface-roughness (SR)-induced variability at low supply voltage [Formula Omitted] in nanowire InAs tunnel FETs and...
We present a comparative study of the surface-roughness (SR)-induced variability at low supply voltage ... in nanowire InAs tunnel FETs and strained-silicon...
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SubjectTerms Applied sciences
Cross-disciplinary physics: materials science; rheology
Devices
Electronics
Exact sciences and technology
Indium arsenides
Materials science
MOSFETs
Nanocomposites
Nanomaterials
Nanoscale materials and structures: fabrication and characterization
Nanostructure
Nanowires
Physics
Quantum wires
Rough surfaces
Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices
Silicon
Strontium
Surface roughness
Three dimensional
Transistors
tunnel-FET
Tunneling
Tunnels (transportation)
variability
Title Surface-Roughness-Induced Variability in Nanowire InAs Tunnel FETs
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