Modulating the Surface State of SiC to Control Carrier Transport in Graphene/SiC
Source abstract
Abstract
Abstract Silicon carbide (SiC) with epitaxial graphene (EG/SiC) shows a great potential in the applications of electronic and photoelectric devices. The performance of devices is primarily dependent on the interfacial heterojunction between graphene and SiC. Here, the band structure of the EG/SiC heterojunction is experimentally investigated by Kelvin probe force microscopy. The dependence of the barrier height at the EG/SiC heterojunction to the initial surface state of SiC is revealed. Both the barrier height and band bending tendency of the heterojunction can be modulated by controlling the surface state of SiC, leading to the tuned carrier transport behavior at the EG/SiC interface. The barrier height at the EG/SiC(000‐1) interface is almost ten times that of the EG/SiC(0001) interface. As a result, the amount of carrier transport at the EG/SiC(000‐1) interface is about ten times that of the EG/SiC(0001) interface. These results offer insights into the carrier transport behavior at the EG/SiC heterojunction by controlling the initial surface state of SiC, and this strategy can be extended in all devices with graphene as the top layer.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Graphene research and applications · Diamond and Carbon-based Materials Research · Silicon Carbide Semiconductor Technologies
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
State Key Laboratory of Luminescence and Applications Changchun Institute of Optics Fine Mechanics and Physics Chinese Academy of Sciences Changchun 130033 P. R. China
University of Chinese Academy of Sciences Beijing 100039 P. R. China
Funding
National Natural Science Foundation of China · Youth Innovation Promotion Association of the Chinese Academy of Sciences
References (35)
Show source-provided references
1. 10.1126/science.118428910.1126/science.1184289 ↗
2. 10.1021/nl303587r10.1021/nl303587r ↗
3. 10.1109/LED.2009.202069910.1109/LED.2009.2020699 ↗
4. 10.1021/nl102824h10.1021/nl102824h ↗
5. 10.7567/APEX.8.04130110.7567/APEX.8.041301 ↗
6. 10.1088/0022-3727/48/9/09510410.1088/0022-3727/48/9/095104 ↗
7. 10.1063/1.494038510.1063/1.4940385 ↗
8. 10.1126/science.112592510.1126/science.1125925 ↗
9. 10.1038/nphoton.2010.18610.1038/nphoton.2010.186 ↗
10. 10.1038/lsa.2016.5210.1038/lsa.2016.52 ↗
11. 10.1002/adma.20150353410.1002/adma.201503534 ↗
12. 10.1002/smll.20170339110.1002/smll.201703391 ↗
13. 10.1116/1.348096110.1116/1.3480961 ↗
14. 10.1109/TED.2008.92659310.1109/TED.2008.926593 ↗
15. 10.1021/nl900803z10.1021/nl900803z ↗
16. 10.1103/PhysRevB.84.23542610.1103/PhysRevB.84.235426 ↗
17. 10.1002/anie.20120041310.1002/anie.201200413 ↗
18. 10.1016/j.carbon.2012.09.00810.1016/j.carbon.2012.09.008 ↗
19. 10.1007/s12274-013-0317-710.1007/s12274-013-0317-7 ↗
20. 10.1103/PhysRevB.79.16140510.1103/PhysRevB.79.161405 ↗
21. 10.1088/0022-3727/45/15/15400310.1088/0022-3727/45/15/154003 ↗
22. 10.1063/1.295308110.1063/1.2953081 ↗
23. 10.1016/j.jcrysgro.2012.04.02510.1016/j.jcrysgro.2012.04.025 ↗
24. 10.1063/1.351154110.1063/1.3511541 ↗
25. 10.1021/nl400043q10.1021/nl400043q ↗
26. 10.1063/1.292974610.1063/1.2929746 ↗
27. 10.1016/j.physrep.2009.02.00310.1016/j.physrep.2009.02.003 ↗
28. 10.1002/adma.20130294110.1002/adma.201302941 ↗
29. 10.1002/aelm.20150025510.1002/aelm.201500255 ↗
30. 10.1103/PhysRevB.80.08542410.1103/PhysRevB.80.085424 ↗
31. 10.1103/PhysRevB.77.12541610.1103/PhysRevB.77.125416 ↗
32. 10.1002/pssa.20153290910.1002/pssa.201532909 ↗
33. 10.1038/lsa.2017.3810.1038/lsa.2017.38 ↗
34. 10.1021/nn204604m10.1021/nn204604m ↗
35. 10.1021/nl301863e10.1021/nl301863e ↗