Ambipolar Charge Transport in Two-Dimensional WS2 Metal–Insulator–Semiconductor and Metal–Insulator–Semiconductor Field-Effect Transistors
Source abstract
Abstract
Two-dimensional (2D) materials with ambipolar transport characteristics have attracted considerable attention as post-complementary metal–oxide semiconductor (CMOS) materials. These materials allow for electron- or hole-dominant conduction to be achieved in a single channel of the field-effect transistors (FETs) without an extrinsic doping. In this study, all-2D metal–insulator–semiconductor (MIS)-based devices, which were composed of all-2D graphene, hexagonal boron nitride, and WS 2, exhibited ambipolar and symmetrical transport characteristics with a low surface state density ( D it, min ≈ 7 × 10 11 cm –2 ·eV –1 ). Hole- or electron-dominant inversion under the influence of electrostatic doping was obtained in a WS 2 -based 2D capacitor up to a frequency range of 1 MHz. n- and p-channel conductions with enhancement-mode operations were selectively realized in a single MISFET, which presented a current on/off ratio of >10 6 and high field-effect mobility (μ e = 58–67 cm 2 /V·s and μ h = 19–30 cm 2 /V·s). Furthermore, a monolithic CMOS-like logic inverter, which employed a single WS 2 flake, exhibited a high gain of 78. These results can be used to reduce the footprints of the device architectures and simplify the device fabrication processes of next-generation CMOS integrated circuits.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Graphene research and applications · 2D Materials and Applications · MXene and MAX Phase Materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Chemical and Biological Engineering, Korea University, Seoul 02841, Korea
Funding
National Research Foundation of Korea · Korea Institute of Energy Technology Evaluation and Planning
References (35)
Show source-provided references
1. 10.1038/nnano.2014.20710.1038/nnano.2014.207 ↗
2. Pierret R. F. · 1996
3. Campbell S. A. · 2008
4. 10.1002/adma.20170179810.1002/adma.201701798 ↗
5. 10.1002/adma.20130584510.1002/adma.201305845 ↗
6. 10.1016/j.sse.2009.04.00210.1016/j.sse.2009.04.002 ↗
7. 10.1021/nl202157510.1021/nl2021575 ↗
8. 10.1021/nn505868h10.1021/nn505868h ↗
9. 10.1002/adma.20110141010.1002/adma.201101410 ↗
10. 10.1002/adfm.20190210510.1002/adfm.201902105 ↗
11. 10.1021/nl803066v10.1021/nl803066v ↗
12. 10.1126/science.287.5455.102210.1126/science.287.5455.1022 ↗
13. 10.1126/science.aac943910.1126/science.aac9439 ↗
14. 10.1039/c8cs90048e10.1039/c8cs90048e ↗
15. 10.1088/2053-1583/3/2/02200110.1088/2053-1583/3/2/022001 ↗
16. 10.1038/natrevmats.2016.4210.1038/natrevmats.2016.42 ↗
17. 10.1063/1.482040810.1063/1.4820408 ↗
18. 10.1021/nl500171v10.1021/nl500171v ↗
19. 10.1063/1.491640310.1063/1.4916403 ↗
20. 10.1063/1.473252210.1063/1.4732522 ↗
21. 10.1109/led.2017.267385410.1109/led.2017.2673854 ↗
22. 10.1021/acsami.6b0156810.1021/acsami.6b01568 ↗
23. 10.1038/srep4066910.1038/srep40669 ↗
24. 10.1021/nl302389d10.1021/nl302389d ↗
25. 10.1109/ted.2011.215922110.1109/ted.2011.2159221 ↗
26. 10.1038/srep1069910.1038/srep10699 ↗
27. 10.1109/ted.2018.284723010.1109/ted.2018.2847230 ↗
28. 10.1103/physrevlett.97.18740110.1103/physrevlett.97.187401 ↗
29. 10.1016/j.vacuum.2016.12.02310.1016/j.vacuum.2016.12.023 ↗
30. 10.1016/0022-4596(87)90057-010.1016/0022-4596(87)90057-0 ↗
31. 10.1016/s1369-7021(13)70014-210.1016/s1369-7021(13)70014-2 ↗
32. Nicollian E. H. · 2002
33. 10.1063/1.504009310.1063/1.5040093 ↗
34. 10.1038/s41699-018-0050-x10.1038/s41699-018-0050-x ↗
35. Sze S. M. · 200610.1002/0470068329 ↗