Controlling Carrier Type and Concentration in NiO Films To Enable in Situ PN Homojunctions
Source abstract
Abstract
The oxygen partial pressure during NiO deposition in reactive sputtering of a Ni target is used to control its carrier type and concentration, obtaining both n- and p-type films. Carrier concentration can be controlled, ranging from 1019 to 1014 cm-3. Films deposition is performed at 200 °C, a relatively low temperature that enables the use of glass as substrate. Experimental band diagrams for n-type NiO are obtained for the first time. Finally, a NiO homojunction is demonstrated by introducing a low carrier concentration layer in between n- and p+-type NiO layers. Layers are deposited in situ, preventing contamination and improving the interface quality, as observed by TEM. The Ni:O ratio for each layer was also obtained by analytical TEM measurements, demonstrating the impact of the oxygen partial pressure on the films' stoichiometry and the simplicity of our process to control carrier type and carrier concentration in oxide semiconductors.
Source: europepmc · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: ZnO doping and properties · Transition Metal Oxide Nanomaterials · Ga2O3 and related materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Materials Science and Engineering, The University of Texas at Dallas, 800 W. Campbell Road, Richardson, Texas 75080, United States
Institute for Microelectronics and Microsystems, CNR-IMM, Via Monteroni, 73100 Lecce, Italy
Funding
Division of Industrial Innovation and Partnerships · Air Force Office of Scientific Research · Consejo Nacional de Ciencia y Tecnolog?a
References (42)
Show source-provided references
1. 10.1002/jsid.65110.1002/jsid.651 ↗
2. 10.1088/0022-3727/49/21/21300110.1088/0022-3727/49/21/213001 ↗
3. 10.1088/1361-6641/aaa7a610.1088/1361-6641/aaa7a6 ↗
4. 10.1021/nl504701y10.1021/nl504701y ↗
5. 10.1002/adma.20150052310.1002/adma.201500523 ↗
6. 10.1016/j.physe.2008.10.01310.1016/j.physe.2008.10.013 ↗
7. 10.1016/S0040-6090(03)01178-710.1016/S0040-6090(03)01178-7 ↗
8. 10.1021/acsami.8b0809510.1021/acsami.8b08095 ↗
9. 10.1016/j.surfcoat.2004.10.03210.1016/j.surfcoat.2004.10.032 ↗
10. Reddy Y. · J. Nano-Electron. Phys. · 2012 · 4 · 04002
11. 10.1039/C4TA06425A10.1039/C4TA06425A ↗
12. 10.1063/1.495346010.1063/1.4953460 ↗
13. 10.1016/0040-6090(93)90636-410.1016/0040-6090(93)90636-4 ↗
14. 10.1016/j.mssp.2017.09.02110.1016/j.mssp.2017.09.021 ↗
15. 10.1109/AM-FPD.2015.717321810.1109/AM-FPD.2015.7173218 ↗
16. 10.1016/j.electacta.2008.08.02710.1016/j.electacta.2008.08.027 ↗
17. 10.1016/S0042-207X(98)00011-610.1016/S0042-207X(98)00011-6 ↗
18. 10.1116/1.151799710.1116/1.1517997 ↗
19. 10.1351/pac19946606131110.1351/pac199466061311 ↗
20. 10.1039/c1ja10087d10.1039/c1ja10087d ↗
21. 10.1016/j.tsf.2007.07.03510.1016/j.tsf.2007.07.035 ↗
22. 10.1021/cg401408f10.1021/cg401408f ↗
23. 10.1557/jmr.2012.44310.1557/jmr.2012.443 ↗
24. 10.1063/1.367141210.1063/1.3671412 ↗
25. 10.1002/pssa.20077891410.1002/pssa.200778914 ↗
26. 10.1016/S0022-0248(02)01753-010.1016/S0022-0248(02)01753-0 ↗
27. Weber D. · Forschungszentrum Jülich · 2014
28. Kasap S. O. · 2006 · 2
29. 10.1039/c3cc48877b10.1039/c3cc48877b ↗
30. 10.1016/j.tsf.2011.10.05910.1016/j.tsf.2011.10.059 ↗
31. 10.1016/j.orgel.2010.05.00810.1016/j.orgel.2010.05.008 ↗
32. 10.1116/1.124775110.1116/1.1247751 ↗
33. 10.1088/0268-1242/20/8/02710.1088/0268-1242/20/8/027 ↗
34. 10.1002/sia.164010.1002/sia.1640 ↗
35. 10.1088/0268-1242/31/5/05501610.1088/0268-1242/31/5/055016 ↗
36. 10.1016/j.susc.2006.01.04110.1016/j.susc.2006.01.041 ↗
37. 10.1016/S0925-4005(01)00802-410.1016/S0925-4005(01)00802-4 ↗
38. 10.1364/OE.23.02768310.1364/OE.23.027683 ↗
39. 10.1063/1.159862410.1063/1.1598624 ↗
40. 10.7567/APEX.9.09110110.7567/APEX.9.091101 ↗
41. 10.1109/LED.2012.222365310.1109/LED.2012.2223653 ↗
42. 10.1088/1361-6463/aaab2c10.1088/1361-6463/aaab2c ↗