Critical Role of Quantum Confinement on Transfer Length in Achieving High-Performance In<sub>2</sub>O<sub>3</sub> Transistors with Ultra-Scaled Contacted Gate Pitch

In this work, for the first time, we study the contact length <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\left(\mathrm{L}_{\mathrm{C}}\right)$</tex> and contacted gate pitch (CGP) scaling in ultrathin <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{In}_{2} \mathrm{O}_{3}$</tex> field-effect transistors (FETs). A large 53 % decrease in transfer length (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{L}_{\mathrm{T}}$</tex>) from 76 to 36 nm can be observed by increasing the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{In}_{2} \mathrm{O}_{3}$</tex> channel thickness (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{T}_{\text{ch}}$</tex>) from 1.2 nm to 2.0 nm, which can be understood by the positive-to-negative Schottky barrier height (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\Phi_{\text{SB}}$</tex>) transition modulated by the quantum confinement (QC) effect in <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{In}_{2} \mathrm{O}_{3}$</tex> channel. Leveraging the record-low <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{L}_{\mathrm{T}}$</tex> of 36 nm optimized by the QC, <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2.0 \text{nm} \text{In}_{2} \mathrm{O}_{3}$</tex> FETs demonstrate a record-low contact resistance (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{R}_{\mathrm{C}}$</tex>) of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$140 \Omega \cdot \mu$</tex> m and a record-high maximum drain current (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{I}_{\mathrm{D}, \max}$</tex>) of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$1.57 \text{mA} / \mu \mathrm{m}$</tex> at ultrascaled CGP of 80 nm among all reported oxide semiconductor FETs with CGP scaling.

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Published
2025-06-08
DOI
https://doi.org/10.23919/vlsitechnologyandcir65189.2025.11074856
Citations
2
Primary Topic
Semiconductor materials and devices
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article
Field-Weighted Citation Impact
1.46
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article

Critical Role of Quantum Confinement on Transfer Length in Achieving High-Performance In2O3 Transistors with Ultra-Scaled Contacted Gate Pitch

Chang Niu, C.H. Liu, Jian-Yu Lin, Peide D. Ye et al.
2 citations
Semiconductor materials and devices
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article

Critical Role of Quantum Confinement on Transfer Length in Achieving High-Performance In2O3 Transistors with Ultra-Scaled Contacted Gate Pitch

Chang Niu, C.H. Liu, Jian-Yu Lin, Peide D. Ye, Zehao Lin, Juanjuan Lu, Haiyan Wang
article en
2 citations

Abstract

In this work, for the first time, we study the contact length <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\left(\mathrm{L}_{\mathrm{C}}\right)$</tex> and contacted gate pitch (CGP) scaling in ultrathin <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{In}_{2} \mathrm{O}_{3}$</tex> field-effect transistors (FETs). A large 53 % decrease in transfer length (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{L}_{\mathrm{T}}$</tex>) from 76 to 36 nm can be observed by increasing the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{In}_{2} \mathrm{O}_{3}$</tex> channel thickness (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{T}_{\text{ch}}$</tex>) from 1.2 nm to 2.0 nm, which can be understood by the positive-to-negative Schottky barrier height (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\Phi_{\text{SB}}$</tex>) transition modulated by the quantum confinement (QC) effect in <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{In}_{2} \mathrm{O}_{3}$</tex> channel. Leveraging the record-low <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{L}_{\mathrm{T}}$</tex> of 36 nm optimized by the QC, <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2.0 \text{nm} \text{In}_{2} \mathrm{O}_{3}$</tex> FETs demonstrate a record-low contact resistance (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{R}_{\mathrm{C}}$</tex>) of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$140 \Omega \cdot \mu$</tex> m and a record-high maximum drain current (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{I}_{\mathrm{D}, \max}$</tex>) of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$1.57 \text{mA} / \mu \mathrm{m}$</tex> at ultrascaled CGP of 80 nm among all reported oxide semiconductor FETs with CGP scaling.

Purdue University West Lafayette (US)
Affordable and clean energy
Openalex Percentile: Top 16%
Semiconductor materials and devices
1.46
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