Ab initio quantum transport simulation of the sub-1 nm gate-length monolayer and bilayer α-MoTe2 field-effect transistors

Abstract

Two-dimensional semiconducting α-MoTe2 is a promising channel material for the field-effect transistors (FETs). Recently, the performance limit of the sub-5 nm gate-length n- and p-type monolayer and multilayer α-MoTe2 transistors has been reported theoretically. However, this material is still unexplored for the ultra-short (sub-1 nm) gate-length n- and p-type metal–oxide semiconductor field-effect transistors (MOSFETs). Here, we performed ab initio quantum transport simulation of the 0.34 nm gate-length n- and p-type MOSFET based on the monolayer (ML) and bilayer (BL) α-MoTe2 for high-performance (HP) and low-power (LP) applications. The proposed n-type ML α-MoTe2 transistor achieves an on-state current (Ion) of 396 μA μm−1 for HP and 183 μA μm−1 for LP, and intrinsic delay time (τ) of 0.334 ps for HP and 1.075 ps for LP. It also exhibits a power delay product (PDP) of 0.071 fJ μm−1 for HP and 0.060 fJ μm−1 for LP, thereby satisfying the International Technology Roadmap for Semiconductors (ITRS) requirements for both HP and LP applications. Unfortunately, the p-type ML and the n and p-type BL α-MoTe2 transistors fail to achieve the required Ion to meet the ITRS standard for HP and LP applications. This research extends the potential application of the ML α-MoTe2 from the sub-5 nm gate-length FETs to the sub-1 nm region.

Graphical abstract: Ab initio quantum transport simulation of the sub-1 nm gate-length monolayer and bilayer α-MoTe2 field-effect transistors

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Article information

Article type
Paper
Submitted
28 Apr 2025
Accepted
25 Jun 2025
First published
30 Jun 2025

J. Mater. Chem. C, 2025, Advance Article

Ab initio quantum transport simulation of the sub-1 nm gate-length monolayer and bilayer α-MoTe2 field-effect transistors

M. Husain, Y. Ahmed, X. Yang, S. Fang, Z. Yang, J. Dong, L. Xu, N. Rahman and J. Lu, J. Mater. Chem. C, 2025, Advance Article , DOI: 10.1039/D5TC01702E

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