journal article·2015-12Open access

High‐Performance, Air‐Stable, Top‐Gate, p‐Channel WSe2 Field‐Effect Transistor with Fluoropolymer Buffer Layer

Seyed Hossein Hosseini Shokouh, Pyo Jin Jeon, Atiye Pezeshki, Kyunghee Choi, Hee Sung Lee, Jin Sung Kim, Eun Young Park, Seongil Im

Advanced Functional Materials· Volume 25· Issue 46

Abstract

High‐performance, air‐stable, p‐channel WSe2 top‐gate field‐effect transistors (FETs) using a bilayer gate dielectric composed of high‐ and low‐k dielectrics are reported. Using only a high‐k Al2O3 as the top‐gate dielectric generally degrades the electrical properties of p‐channel WSe2, therefore, a thin fluoropolymer (Cytop) as a buffer layer to protect the 2D channel from high‐k oxide forming is deposited. As a result, a top‐gate‐patterned 2D WSe2 FET is realized. The top‐gate p‐channel WSe2 FET demonstrates a high hole mobility of 100 cm2­ V−1 s−1 and a ION/IOFF ratio > 107 at low gate voltages (VGS ca. −4 V) and a drain voltage (VDS) of −1 V on a glass substrate. Furthermore, the top‐gate FET shows a very good stability in ambient air with a relative humidity of 45% for 7 days after device fabrication. Our approach of creating a high‐k oxide/low‐k organic bilayer dielectric is advantageous over single‐layer high‐k dielectrics for top‐gate p‐channel WSe2 FETs, which will lead the way toward future electronic nanodevices and their integration.
Source: crossref · Quality: baseline

Research context

OpenAlex topics: 2D Materials and Applications · MXene and MAX Phase Materials · Graphene research and applications

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Institute of Physics and Applied Physics Yonsei University 50 Yonsei‐ro Seodaemun‐gu Seoul 120‐749 Korea

Funding

National Research Foundation of Korea · Brain Korea 21 plus Program

References (44)

Show source-provided references
1. 10.1021/nl304777e10.1021/nl304777e ↗
2. 10.1021/nl501275p10.1021/nl501275p ↗
3. Sahin H. · Phys. Rev. B: Condens. Matter · 2013 · 87 · 165
4. 10.1038/nnano.2014.20710.1038/nnano.2014.207 ↗
5. 10.1021/acsnano.5b0015310.1021/acsnano.5b00153 ↗
6. 10.1021/nn500914810.1021/nn5009148 ↗
7. 10.1021/nl404350510.1021/nl4043505 ↗
8. 10.1103/PhysRevB.87.16540210.1103/PhysRevB.87.165402 ↗
9. 10.1063/1.486719710.1063/1.4867197 ↗
10. 10.1021/nl503251h10.1021/nl503251h ↗
11. 10.1021/nl501531610.1021/nl5015316 ↗
12. 10.1021/nl301485q10.1021/nl301485q ↗
13. 10.1038/nnano.2010.27910.1038/nnano.2010.279 ↗
14. 10.1038/nnano.2012.19310.1038/nnano.2012.193 ↗
15. 10.1063/1.491434910.1063/1.4914349 ↗
16. 10.1038/nnano.2014.2510.1038/nnano.2014.25 ↗
17. 10.1038/nnano.2014.6610.1038/nnano.2014.66 ↗
18. Das S. · Appl. Phys. Lett. · 2013 · 103 · 103
19. 10.1038/nnano.2014.1410.1038/nnano.2014.14 ↗
20. 10.1038/nnano.2014.2610.1038/nnano.2014.26 ↗
21. Das S. · Appl. Phys. Lett. · 2014 · 105 · 083
22. 10.1021/nn500992910.1021/nn5009929 ↗
23. Chen K. · APL Mater. · 2014 · 2 · 092
24. 10.1021/nl400044m10.1021/nl400044m ↗
25. 10.1088/2053-1583/1/3/03400110.1088/2053-1583/1/3/034001 ↗
26. 10.1021/nn507443510.1021/nn5074435 ↗
27. 10.1021/nn504784410.1021/nn5047844 ↗
28. 10.1021/nl301702r10.1021/nl301702r ↗
29. 10.1021/nl504256y10.1021/nl504256y ↗
30. Ma N. · Phys. Rev. X · 2014 · 4 · 011
31. 10.1039/C4TC02961E10.1039/C4TC02961E ↗
32. 10.1002/pssr.20130701510.1002/pssr.201307015 ↗
33. 10.1021/nl401831u10.1021/nl401831u ↗
34. 10.1021/nl303583v10.1021/nl303583v ↗
35. 10.1038/srep0897910.1038/srep08979 ↗
36. 10.1021/jp953676310.1021/jp9536763 ↗
37. 10.1021/nl202239c10.1021/nl202239c ↗
38. 10.1039/C4CP01237B10.1039/C4CP01237B ↗
39. 10.1038/nnano.2013.3010.1038/nnano.2013.30 ↗
40. 10.1039/C4RA17320A10.1039/C4RA17320A ↗
41. 10.1021/am405424k10.1021/am405424k ↗
42. 10.1002/adma.20100427810.1002/adma.201004278 ↗
43. 10.1021/am508723a10.1021/am508723a ↗
44. 10.1021/nl504975310.1021/nl5049753 ↗