Schottky Diode with Asymmetric Metal Contacts on WS2
Source abstract
Abstract
Abstract Diode characteristics of transition metal dichalcogenides are studied extensively owing to their electrical and optical properties. In particular, the Schottky barrier diode (SBD) structure has advantages, such as its small leakage current and power consumption, over conventional p–n diodes. This study develops an SBD system using n‐type tungsten disulfide (WS2). By depositing a low work function In (ΦIn = 4.1 eV) and high work function Au (ΦAu = 5.1 eV) on n‐type WS2, the diode characteristics are demonstrated to be close to an ideal diode. The In–Au contacts are measured, and SBD characteristics are confirmed with a 1.02 ideality factor at a zero back‐gate voltage at room temperature and a rectification ratio up to 5 × 102, even at a low temperature (77 K), indicating almost ideal diode properties. In addition, the In electrodes exhibited improved electrical properties, with a high on/off ratio of 107, mobility that is 100 times higher, and Schottky barrier height that is 20 times lower than that of Au electrodes.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: 2D Materials and Applications · Graphene research and applications · MXene and MAX Phase Materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Electrical and Computer Engineering Sungkyunkwan University (SKKU) Suwon 16419 Republic of Korea
Samsung‐SKKU Graphene Center Sungkyunkwan Advanced Institute of Nanotechnology (SAINT) Sungkyunkwan University (SKKU) Suwon 16419 Republic of Korea
Department of Advanced Materials Science and Engineering Sungkyunkwan University (SKKU) Suwon 16419 Republic of Korea
Funding
National Research Foundation of Korea
References (40)
Show source-provided references
1. 10.1038/nnano.2014.20710.1038/nnano.2014.207 ↗
2. 10.1021/nn502362b10.1021/nn502362b ↗
3. 10.1002/adma.20150222210.1002/adma.201502222 ↗
4. 10.1021/acs.nanolett.6b0477510.1021/acs.nanolett.6b04775 ↗
5. 10.1002/adfm.20160446810.1002/adfm.201604468 ↗
6. 10.1021/acs.jpclett.5b0268710.1021/acs.jpclett.5b02687 ↗
7. 10.1002/smll.20180036510.1002/smll.201800365 ↗
8. 10.1021/nl500171v10.1021/nl500171v ↗
9. 10.1038/nphoton.2015.28210.1038/nphoton.2015.282 ↗
10. 10.1038/s41928-019-0273-710.1038/s41928-019-0273-7 ↗
11. 10.1038/s41699-020-0152-010.1038/s41699-020-0152-0 ↗
12. 10.1126/sciadv.160311310.1126/sciadv.1603113 ↗
13. 10.1038/s41586-018-0013-610.1038/s41586-018-0013-6 ↗
14. 10.1038/nnano.2014.1410.1038/nnano.2014.14 ↗
15. 10.1021/acsnano.5b0318810.1021/acsnano.5b03188 ↗
16. 10.1002/adma.20150409010.1002/adma.201504090 ↗
17. 10.1002/adma.20160194910.1002/adma.201601949 ↗
18. 10.1016/j.nanoen.2018.04.05510.1016/j.nanoen.2018.04.055 ↗
19. 10.1002/adfm.20200336010.1002/adfm.202003360 ↗
20. 10.1039/D0TC04840B10.1039/D0TC04840B ↗
21. 10.1021/acsami.8b0607810.1021/acsami.8b06078 ↗
22. 10.1039/C8RA09656B10.1039/C8RA09656B ↗
23. 10.1038/s41598-017-16251-210.1038/s41598-017-16251-2 ↗
24. 10.1103/PhysRevB.83.24521310.1103/PhysRevB.83.245213 ↗
25. 10.1038/srep2034310.1038/srep20343 ↗
26. 10.1039/C7CS00828G10.1039/C7CS00828G ↗
27. 10.1088/2053-1583/4/1/01500710.1088/2053-1583/4/1/015007 ↗
28. 10.1038/srep0175510.1038/srep01755 ↗
29. 10.1103/PhysRevB.88.16531610.1103/PhysRevB.88.165316 ↗
30. 10.1002/adts.20200010310.1002/adts.202000103 ↗
31. 10.1002/advs.20210010210.1002/advs.202100102 ↗
32. 10.1038/s41586-018-0129-810.1038/s41586-018-0129-8 ↗
33. 10.1021/acs.nanolett.1c0001510.1021/acs.nanolett.1c00015 ↗
34. 10.1039/C8NR10526J10.1039/C8NR10526J ↗
35. 10.1016/j.jallcom.2019.05.02810.1016/j.jallcom.2019.05.028 ↗
36. 10.1088/1361-6641/aae62f10.1088/1361-6641/aae62f ↗
37. 10.1038/s41377-020-00396-310.1038/s41377-020-00396-3 ↗
38. 10.1103/PhysRevApplied.14.05402710.1103/PhysRevApplied.14.054027 ↗
39. 10.1021/acsami.6b1669210.1021/acsami.6b16692 ↗
40. 10.3390/cryst1008063610.3390/cryst10080636 ↗