journal article·2022-03-22Open access

Spectroscopic Ellipsometry Study on Tuning the Electrical and Optical Properties of Zr-Doped ZnO Thin Films Grown by Atomic Layer Deposition

Carolina Bohórquez, Hicham Bakkali, Juan J. Delgado, Eduardo Blanco, Manuel Herrera, Manuel Domínguez

Abstract

This work reports the ellipsometry analysis of atomic layer deposition (ALD) films of ZnO doped with Zr to determine parameters like free carrier concentration and mobility. Thin films of zinc oxide (ZnO) and Zr-doped ZnO of thickness ∼100 nm were prepared by atomic layer deposition on sapphire, SiO2/Si(100), and Si(100) substrates. Variable-angle spectroscopic ellipsometry was used to study their optical properties in the 0.5–3.5 eV spectral range. The optical constants were accurately obtained using a model that combines Drude and Tauc–Lorentz oscillators with Bruggeman effective medium approximations, allowing the inclusion of a roughness layer in the optical model. The effect of Zr doping (ca. 1.9–4.4 atom %) was then investigated in both as-prepared samples and samples annealed in the temperature range of 100–300 °C. All of the films exhibited good optical transparency (ca. 70–90% in the visible region). For doping levels below 2.7 atom %, the real part of the dielectric permittivity reveals a semiconductor-to-metal transition in the near-infrared (NIR) region, as the permittivity goes from positive to negative. Besides, the plasma energy increases with increasing Zr concentration, and both resistivity and carrier concentration exhibit slightly parabolic behaviors, with a minimum of ∼1.5 × 10–3 Ω cm and a maximum of 2.4 × 1020 cm–3, respectively, at the same critical Zr concentration (2.7 atom %). In contrast, the carrier mobility decreases rapidly from 76.0 to 19.2 cm2/(V s) with increasing Zr content, while conductivities and carrier mobilities worsen when the annealing temperature increases, probably due to the segregation of ZnO crystals. Finally, the optical band gap is very stable, revealing its interesting independence of substrate composition and annealing temperature, as it collapses to a single master curve when band gap energy is plotted versus free carrier concentration, following the Burstein–Moss effect. Overall, the Zr-doped ZnO films studied here would be a highly desirable system for developing thermally stable transparent conductive oxides (TCOs).
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: ZnO doping and properties · Thin-Film Transistor Technologies · Copper-based nanomaterials and applications

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

Affiliations

Centro de Investigación Científica y de Educación Superior de Ensenada (CICESE), 22860 Ensenada, Baja California, Mexico

Departamento de Física de la Materia Condensada, Universidad de Cádiz, Campus de Puerto Real, E11519 Puerto Real, Spain

Institute of Research on Electron Microscopy and Materials (IMEYMAT), Universidad de Cádiz, Campus de Puerto Real, E11519 Puerto Real, Spain

Departamento Ciencias de los Materiales e Ingeniería Metalúrgica y Química Inorgánica, Universidad de Cádiz, Campus de Puerto Real, E11519 Puerto Real, Spain

Centro de Nanociencias y Nanotecnología, Universidad Nacional Autónoma de México, 22860 Ensenada, Baja California, Mexico

Funding

Consejo Nacional de Ciencia y Tecnolog?a · Universidad de C?diz

References (43)

Show source-provided references
1. Bahadur B. · 199210.1142/1300 ↗
2. 10.1016/J.MEE.2009.01.06710.1016/J.MEE.2009.01.067 ↗
3. Li Z. R. · 2006
4. 10.1039/C7RA13550E10.1039/C7RA13550E ↗
5. 10.1039/C1EE01873F10.1039/C1EE01873F ↗
6. 10.1016/J.JALLCOM.2019.04.04210.1016/J.JALLCOM.2019.04.042 ↗
7. 10.1016/J.OPTMAT.2006.08.00210.1016/J.OPTMAT.2006.08.002 ↗
8. 10.1179/1753555715Y.000000004710.1179/1753555715Y.0000000047 ↗
9. 10.1149/2.026204JES10.1149/2.026204JES ↗
10. 10.1021/acs.jpcc.9b0225310.1021/acs.jpcc.9b02253 ↗
11. 10.1016/J.JALLCOM.2007.02.03510.1016/J.JALLCOM.2007.02.035 ↗
12. 10.1016/S0921-5107(02)00622-010.1016/S0921-5107(02)00622-0 ↗
13. 10.1103/PhysRevB.83.08520210.1103/PhysRevB.83.085202 ↗
14. 10.5370/JEET.2013.8.1.16310.5370/JEET.2013.8.1.163 ↗
15. 10.1111/J.1151-2916.1998.TB02524.X10.1111/J.1151-2916.1998.TB02524.X ↗
16. Bundesmann C. · 2008 · 104 · 7910.1007/978-3-540-73612-7_3 ↗
17. Kosyachenko L. A. · 201110.5772/821 ↗
18. 10.1186/1556-276X-8-10810.1186/1556-276X-8-108 ↗
19. Yuan H. · Rengong Jingti Xuebao · 2013 · 42 · 240
20. Fujiwara, H. Spectroscopic Ellipsometry: Principles and Applications; John Wiley & Sons, Ltd., 2007; pp 1–369.10.1002/9780470060193 ↗
21. 10.1103/PhysRevB.71.07510910.1103/PhysRevB.71.075109 ↗
22. 10.1116/6.000018410.1116/6.0000184 ↗
23. 10.1149/1.357516110.1149/1.3575161 ↗
24. 10.3390/ma810536910.3390/ma8105369 ↗
25. 10.3390/MA908069510.3390/MA9080695 ↗
26. 10.1109/TED.2019.289631310.1109/TED.2019.2896313 ↗
27. 10.1002/SOLR.20200024110.1002/SOLR.202000241 ↗
28. 10.1016/J.TSF.2018.06.04510.1016/J.TSF.2018.06.045 ↗
29. 10.1021/JP305747710.1021/JP3057477 ↗
30. 10.1016/S0304-3991(98)00009-610.1016/S0304-3991(98)00009-6 ↗
31. Johs, B.; Woollam, J. A.; Herzinger, C. M.; Hilfiker, J. N.; Synowicki, R. A.; Bungay, C. L. In Overview of Variable-Angle Spectroscopic Ellipsometry (VASE): II. Advanced Applications, SPIE’s International Symposium on Optical Science, Engineering, and Instrumentation, 1999, Denver, 1999.10.1117/12.351667 ↗
32. Cullity B. · 1956
33. 10.1023/B:JMSC.0000017786.81842.AE10.1023/B:JMSC.0000017786.81842.AE ↗
34. 10.1016/J.JKSUS.2016.03.00110.1016/J.JKSUS.2016.03.001 ↗
35. 10.1063/1.11806410.1063/1.118064 ↗
36. 10.1021/acs.jpcc.7b0894310.1021/acs.jpcc.7b08943 ↗
37. 10.1038/s41598-019-47670-y10.1038/s41598-019-47670-y ↗
38. Fujiwara H. · 2018 · 212 · 52310.1007/978-3-319-75377-5_18 ↗
39. 10.1016/J.SOLENER.2019.11.09410.1016/J.SOLENER.2019.11.094 ↗
40. 10.1088/1361-6528/ABA65B10.1088/1361-6528/ABA65B ↗
41. 10.1016/J.APCATB.2009.01.01010.1016/J.APCATB.2009.01.010 ↗
42. 10.1103/PhysRevB.37.1024410.1103/PhysRevB.37.10244 ↗
43. 10.1063/1.36737510.1063/1.367375 ↗