Issue 37, 2023

Anisotropic charge transfer and gate tuning for p-SnS/n-MoS2 vertical van der Waals diodes

Abstract

2D-material-based van der Waals heterostructures (vdWhs) have shown great potential in next-generation multi-functional microelectronic devices. Thanks to their sharp interface and ultrathin thickness, 2D p–n junctions with high rectification properties have been established by combining p-type monochalcogenides with n-type transition metal dichalcogenides. However, the anisotropic rectification together with the charge transfer and gate effect has not been clarified. Herein, the electrical anisotropy of p-SnS/n-MoS2 diodes was studied. Optimum ideality factors within 1.08–1.18 have been achieved for the diode with 6.6 nm thick SnS on monolayer MoS2, and a high rectification ratio of 3.1 × 104 with strong in-plane anisotropy is observed along the zigzag direction of SnS. A strong gate effect on the anisotropic series resistance has been verified and an effective tuning over the transport length of the SnS channel can be established through adjustment of the current orientation and gate voltage. A thickness-dependent minority carrier transport mechanism has also been demonstrated for the reverse drain current, and Fowler–Nordheim tunneling and direct tunneling are proposed for the increase of the reverse current of the thicker and thinner diodes, respectively. This work will provide another strategy for high-performance diodes based on vdWhs via the control of the current orientation and the gate effect.

Graphical abstract: Anisotropic charge transfer and gate tuning for p-SnS/n-MoS2 vertical van der Waals diodes

Supplementary files

Article information

Article type
Paper
Submitted
19 Jul 2023
Accepted
31 Aug 2023
First published
01 Sep 2023

Nanoscale, 2023,15, 15344-15351

Anisotropic charge transfer and gate tuning for p-SnS/n-MoS2 vertical van der Waals diodes

H. Yuan, R. Xu, J. Ren, J. Yang, S. Wang, D. Tian, Y. Fu, Q. Li, X. Peng and X. Wang, Nanoscale, 2023, 15, 15344 DOI: 10.1039/D3NR03508E

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