5 nm Gate length field-effect transistors based on monolayer α-In2X3 (X = S, Se, Te)

Abstract

Recently, α-In2X3 (X = S, Se, and Te) two-dimensional (2D) ferroelectric semiconductors have emerged as a research focus due to their ferroelectricity. However, the potential of their semiconductivity for future field-effect transistors (FETs) remains unclear. Herein, this work quantifies the performance limit of 5 nm gate length (Lg) monolayer (ML) α-In2X3 double-gate (DG) metal–oxide–semiconductor field-effect transistors (MOSFETs) and compares the performance of these devices with non-underlap (non-UL) and symmetric underlap (UL) configurations, using first-principles quantum-transport simulation. For the devices with non-UL configurations, the α-In2S3 MOSFET demonstrates both the highest on-state current (Ion) and the lowest subthreshold swing (SS). Meanwhile, the α-In2Se3 MOSFET shows a low SS, and the α-In2Te3 MOSFET shows a high Ion. Due to the influence of effective mass and bandgap energy, n-type ML α-In2S3 and α-In2Te3 MOSFETs demonstrate superior Ion compared to their α-In2Se3 counterparts. For the devices with UL configurations, the Ion of all ML α-In2X3 DG MOSFETs can meet the International Technology Roadmap for Semiconductors (ITRS) high-performance (HP) and low-power (LP) standards for 2028. Moreover, all ML α-In2X3 DG MOSFETs achieve ideal SS with the aid of the UL. These results indicate that ML α-In2X3 is a viable candidate for future MOSFET channel materials.

Graphical abstract: 5 nm Gate length field-effect transistors based on monolayer α-In2X3 (X = S, Se, Te)

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Article information

Article type
Paper
Submitted
26 Jun 2025
Accepted
18 Sep 2025
First published
19 Sep 2025

Phys. Chem. Chem. Phys., 2025, Advance Article

5 nm Gate length field-effect transistors based on monolayer α-In2X3 (X = S, Se, Te)

Y. Zhong, J. Dai, J. Yuan, D. Deng and M. Zhao, Phys. Chem. Chem. Phys., 2025, Advance Article , DOI: 10.1039/D5CP02433A

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