Machine-Learned Fermi Level Prediction of Solution-Processed Ultrawide-Bandgap Amorphous Gallium Oxide (a-Ga2Ox)
Source abstract
Abstract
The Fermi level (EF) relative position to the conduction band minimum is a crucial consideration for controlling electrical conductivity and semiconductor device performance in thin-film transistors, sensors, and photodetectors. Experiment complexity and expensive material resources for predicting EF via an experimental approach render a machine learning (ML) approach to be more appropriate. This work presents ML-assisted EF prediction of solution-processed ultrawide-bandgap (UWB) amorphous gallium oxide (a-Ga2Ox). Three regression models─kernel ridge regression, support vector regression, and random forest regression─were trained with experimental features including the film thickness, baking temperature, and gas environment during solution deposition of the a-Ga2Ox film. The results show that ML models can be used to predict EF of the UWB a-Ga2Ox film and also identify optimized fabrication parameters to achieve the optimized EF. Moreover, the ML approach can significantly accelerate the fabrication of semiconducting UWB a-Ga2Ox-based material for future device applications. This work is a big step toward rapid and cost-effective optimization methods for developing UWB a-Ga2Ox-based devices.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Ga2O3 and related materials · ZnO doping and properties · Gas Sensing Nanomaterials and Sensors
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Division of Materials Science, Nara Institute of Science and Technology, Nara 630-0192, Japan
Division of Information Science, Nara Institute of Science and Technology, Nara 630-0192, Japan
Department of Computer Science, University of the Philippines Diliman, Quezon City 1101, Philippines
Data Science Center, Nara Institute of Science and Technology, Nara 630-0192, Japan
Funding
Nara Institute of Science and Technology
References (37)
Show source-provided references
1. 10.1002/adma.20200623010.1002/adma.202006230 ↗
2. 10.1002/adfm.20180767210.1002/adfm.201807672 ↗
3. 10.1002/adfm.20170026410.1002/adfm.201700264 ↗
4. 10.1021/acs.jpclett.9b0279310.1021/acs.jpclett.9b02793 ↗
5. 10.1002/pssa.20200033910.1002/pssa.202000339 ↗
6. 10.1063/1.500694110.1063/1.5006941 ↗
7. 10.1021/acsami.9b1169410.1021/acsami.9b11694 ↗
8. 10.35848/1882-0786/ac466a10.35848/1882-0786/ac466a ↗
9. 10.1038/am.2017.2010.1038/am.2017.20 ↗
10. 10.1002/aelm.20190038910.1002/aelm.201900389 ↗
11. 10.1021/acsphotonics.7b0105410.1021/acsphotonics.7b01054 ↗
12. 10.1021/acsphotonics.7b0035910.1021/acsphotonics.7b00359 ↗
13. 10.1002/adom.20170045410.1002/adom.201700454 ↗
14. 10.1021/acsaelm.0c0034810.1021/acsaelm.0c00348 ↗
15. 10.1021/acsami.7b1601010.1021/acsami.7b16010 ↗
16. 10.1016/j.jallcom.2011.08.03310.1016/j.jallcom.2011.08.033 ↗
17. 10.1038/s41524-020-0296-710.1038/s41524-020-0296-7 ↗
18. 10.1016/j.ijleo.2020.16446910.1016/j.ijleo.2020.164469 ↗
19. 10.1016/j.carbon.2016.03.00510.1016/j.carbon.2016.03.005 ↗
20. 10.1038/srep2095210.1038/srep20952 ↗
21. 10.1103/PhysRevMaterials.2.11380310.1103/PhysRevMaterials.2.113803 ↗
22. 10.1080/21642583.2014.95626510.1080/21642583.2014.956265 ↗
23. 10.1177/1536867X2090968810.1177/1536867X20909688 ↗
24. 10.1088/1361-6528/aa82e510.1088/1361-6528/aa82e5 ↗
25. 10.1002/adfm.20190604010.1002/adfm.201906040 ↗
26. 10.1109/TED.2013.226532610.1109/TED.2013.2265326 ↗
27. 10.1021/am100298p10.1021/am100298p ↗
28. 10.1109/TED.2014.235973910.1109/TED.2014.2359739 ↗
29. 10.1557/jmr.2012.19910.1557/jmr.2012.199 ↗
30. 10.1063/1.357064110.1063/1.3570641 ↗
31. 10.1016/j.microrel.2011.07.01810.1016/j.microrel.2011.07.018 ↗
32. 10.1016/j.cap.2014.04.01110.1016/j.cap.2014.04.011 ↗
33. 10.1002/admt.20200094510.1002/admt.202000945 ↗
34. 10.1016/j.apsusc.2018.09.23610.1016/j.apsusc.2018.09.236 ↗
35. 10.1016/j.tsf.2004.11.22310.1016/j.tsf.2004.11.223 ↗
36. 10.1016/j.jallcom.2019.15305210.1016/j.jallcom.2019.153052 ↗
37. 10.1007/s10854-021-05408-510.1007/s10854-021-05408-5 ↗