Evidence for oxygen being a dominant shallow acceptor in p-type CuI
Source abstract
Abstract
For every semiconducting material, the long-term stability of thin film characteristics is a crucial necessity for device applications. This is particularly true for the p-type semiconductor CuI, where the thin film properties are especially sensitive to environmental influences and motivate the application of capping materials. Utilizing pulsed laser deposition (PLD) and Al2O3 cappings, we performed systematic studies on the N2/O2 partial pressure during growth and the effect of layer thickness. Our results suggest that oxygen, acting as an acceptor, and its diffusion through Al2O3 and CuI dominate the conductivity of PLD grown CuI thin films. The diffusion process of atmospheric oxygen into CuI was traced with 18O-isotopes. Additionally, the transparency and morphology of CuI films are also affected by the oxygen supply during capping growth. These results challenge the currently accepted idea that intrinsic, and not extrinsic, effects determine the conductivity of CuI thin films.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: ZnO doping and properties · Copper-based nanomaterials and applications · Electronic and Structural Properties of Oxides
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Felix Bloch Institute for Solid State Physics, Universität Leipzig 1 , Linnéstraße 5, 04103 Leipzig, Germany
Fraunhofer Institute for Microstructure of Materials and Systems IMWS 2 , Walter-Hülse-Straße 1, 06120 Halle, Germany
Funding
Deutsche Forschungsgemeinschaft
References (34)
Show source-provided references
1. Cuprous iodide–A p-type transparent semiconductor: History and novel applications10.1002/pssa.201329349 ↗
2. Growth strategy and physical properties of the high mobility p-type CuI crystal10.1021/cg100270d ↗
3. Highly-transparent and conductive CuI films obtained by a redirected low-cost and electroless two-step route: Chemical solution deposition of CuS2 and subsequent iodination10.1016/j.mssp.2019.02.016 ↗
4. Transparent flexible thermoelectric material based on non-toxic earth-abundant p-type copper iodide thin film10.1038/ncomms16076 ↗
5. Native p-type transparent conductive CuI via intrinsic defects10.1063/1.3633220 ↗
6. First-principles study of γ-CuI for p-type transparent conducting materials10.1088/0022-3727/45/14/145102 ↗
7. Exciton luminescence of CuCl, CuBr and CuI single crystals10.1143/jpsj.24.314 ↗
8. The high-temperature structural behaviour of copper(I) iodide10.1088/0953-8984/7/29/007 ↗
9. High-pressure phase of copper(I) iodide10.1103/physrevb.51.12022 ↗
10. Violet light-emitting diodes based on p-CuI thin film/n-MgZnO quantum dot heterojunction10.1021/acsami.9b18507 ↗
11. Room-temperature solution-synthesized p-type copper(I) iodide semiconductors for transparent thin-film transistors and complementary electronics10.1002/adma.201870258 ↗
12. Hole transport modulations in low dimensional γ-CuI films: Implication for high figure of merit and thin film transistors10.1021/acsaelm.9b00177 ↗
13. High-performance p-channel transistors with transparent Zn doped-CuI10.1038/s41467-020-18006-6 ↗
14. Über die elektrische Leitfähigkeit und die thermoelektrische Kraft einiger Schwermetallverbindungen10.1002/andp.19073270409 ↗
15. Low-temperature fabrication and performance of polycrystalline CuI films as transparent p-type semiconductors10.1002/pssa.201700782 ↗
16. Highly transparent and conductive γ-CuI films grown by simply dipping copper films into iodine solution10.1016/j.physb.2019.08.021 ↗
17. Effect of deposition temperature on transparent conductive properties of γ-CuI film prepared by vacuum thermal evaporation10.1002/pssa.201532015 ↗
18. Room-temperature domain-epitaxy of copper iodide thin films for transparent CuI/ZnO heterojunctions with high rectification ratios larger than 10910.1038/srep21937 ↗
19. Molecular beam epitaxy of high-quality CuI thin films on a low temperature grown buffer layer10.1063/5.0007389 ↗
20. High mobility, highly transparent, smooth, p-type CuI thin films grown by pulsed laser deposition10.1063/5.0021781 ↗
21. Computational acceleration of prospective dopant discovery in cuprous iodide10.1039/c9cp02711d ↗
22. First-Principles study on doping of copper halides10.3938/jkps.77.764 ↗
23. Growth regimes in pulsed laser deposition of aluminum oxide films10.1007/s00339-008-4720-y ↗
24. Influence of oxygen pressure on growth of Si-doped β-(AlxGa1−x)2O3 thin films on c-sapphire substrates by pulsed laser deposition10.1149/2.0411907jss ↗
25. Dissociative chemisorption of O2 on Al(111): Dynamics on a correlated wave-function-based potential energy surface10.1021/acs.jpclett.8b01470 ↗
26. Oxygen molecule dissociation on the Al(111) surface10.1103/physrevlett.84.705 ↗
27. Dissociative sticking of O2 on Al(111)10.1103/physrevb.55.15452 ↗
28. Self-diffusion of oxygen in single crystal and polycrystalline aluminum oxide10.1063/1.1731170 ↗
29. Comparative studies on oxygen diffusion coefficients for Amorphous and γ-Al2O3 films using 18O isotope10.1143/jjap.42.7205 ↗
30. Diffusion of oxygen in amorphous Al2O3, Ta2O5, and Nb2O510.1063/1.4889800 ↗
31. A review of the segmented-target approach to combinatorial material synthesis by pulsed-laser deposition10.1002/pssb.201900626 ↗
32. The matrix effect in TOF-SIMS analysis of two-element inorganic thin films10.1039/c9ja00428a ↗
33. Hybrid organic/inorganic materials depth profiling using low energy cesium ions10.1007/s13361-016-1353-9 ↗
34. 2017 · 1