journal article·2018-01-18

Wannier Koopmans Method Calculations of 2D Material Band Gaps

Mouyi Weng, Sibai Li, Jiaxin Zheng, Feng Pan, Lin-Wang Wang

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Abstract

A major drawback of the widely successful density functional theory is its underestimation of the material band gap. Various methods have been proposed to correct its band gap predictions. Wannier Koopmans method (WKM) is recently developed for this purpose to predict the band gap of extended 3D bulk systems. While the WKM has also been shown to be successful for isolated molecules, it is still a question whether it will work for 2D materials that are in between the 0D molecules and 3D bulk systems. We apply the WKM to 16 commonly known well studied 2D materials and find that the WKM predicted band gaps are on par with their GW calculated results.
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Research context

OpenAlex topics: 2D Materials and Applications · Gas Sensing Nanomaterials and Sensors · Ga2O3 and related materials

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

Affiliations

School of Advanced Materials, Peking University, Shenzhen Graduate School, Shenzhen 518055, People’s Republic of China

Materials Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States

Funding

Ministry of Science and Technology of the People's Republic of China · Basic Energy Sciences · Shenzhen Science and Technology Innovation Committee

References (32)

Show source-provided references
1. 10.1021/cr300263a10.1021/cr300263a ↗
2. 10.1021/nn400280c10.1021/nn400280c ↗
3. 10.1021/acsami.7b0851310.1021/acsami.7b08513 ↗
4. 10.1021/acs.jpcc.6b0269610.1021/acs.jpcc.6b02696 ↗
5. 10.1021/acsami.6b0739010.1021/acsami.6b07390 ↗
6. 10.1021/acsami.6b1523510.1021/acsami.6b15235 ↗
7. 10.1021/nl400600x10.1021/nl400600x ↗
8. 10.1016/j.electacta.2017.01.05910.1016/j.electacta.2017.01.059 ↗
9. 10.1038/nnano.2012.9510.1038/nnano.2012.95 ↗
10. 10.1103/PhysRevLett.55.141810.1103/PhysRevLett.55.1418 ↗
11. 10.1103/PhysRevLett.111.21680510.1103/PhysRevLett.111.216805 ↗
12. 10.1103/PhysRev.140.A113310.1103/PhysRev.140.A1133 ↗
13. 10.1016/0927-0256(96)00008-010.1016/0927-0256(96)00008-0 ↗
14. 10.1021/j100096a00110.1021/j100096a001 ↗
15. 10.1021/j100091a02410.1021/j100091a024 ↗
16. 10.1063/1.499674310.1063/1.4996743 ↗
17. 10.1038/srep2492410.1038/srep24924 ↗
18. 10.1021/jp022577410.1021/jp0225774 ↗
19. 10.1063/1.495512810.1063/1.4955128 ↗
20. 10.1038/srep2178610.1038/srep21786 ↗
21. 10.1103/PhysRevB.95.03513910.1103/PhysRevB.95.035139 ↗
22. 10.1063/1.481232310.1063/1.4812323 ↗
23. 10.1016/j.cpc.2012.08.00210.1016/j.cpc.2012.08.002 ↗
24. 10.1016/j.jcp.2013.05.00510.1016/j.jcp.2013.05.005 ↗
25. 10.1103/PhysRevB.88.08511710.1103/PhysRevB.88.085117 ↗
26. 10.1016/j.cpc.2015.05.01110.1016/j.cpc.2015.05.011 ↗
27. 10.1103/PhysRevB.13.518810.1103/PhysRevB.13.5188 ↗
28. 10.1103/PhysRevB.65.03510910.1103/PhysRevB.65.035109 ↗
29. 10.1021/acs.jpcc.5b0295010.1021/acs.jpcc.5b02950 ↗
30. 10.1063/1.481651710.1063/1.4816517 ↗
31. 10.1103/PhysRevB.93.23543510.1103/PhysRevB.93.235435 ↗
32. 10.1103/PhysRevB.86.11540910.1103/PhysRevB.86.115409 ↗