Comparative study of ITO layers deposited by DC and RF magnetron sputtering at room temperature

被引:147
作者
Kurdesau, F.
Khripunov, G.
da Cunha, A. F.
Kaelin, M.
Tiwari, A. N.
机构
[1] Univ Aveiro, Dept Fis, P-3810193 Aveiro, Portugal
[2] NAS Belarus, Inst Elect, Minsk 220090, BELARUS
[3] Kharkov State Polytech Univ, UA-310002 Kharkov, Ukraine
[4] ETH, Solid State Phys Lab, Thin Film Phys Grp, CH-8005 Zurich, Switzerland
[5] Univ Loughborough, CREST, Dept Elect & Elect Engn, Loughborough LE11 3TU, Leics, England
关键词
II-VI semiconductors; photovoltaics; indium tin oxide and other transparent conductors;
D O I
10.1016/j.jnoncrysol.2005.11.088
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Two different magnetron sputtering techniques with RF and DC plasma discharge modes were tested for room temperature deposition of ITO layers from In-2-O-3:SnO2 targets (10 wt% SnO2). The influence of sputtering conditions (mainly the sputtering power and oxygen content in the Ar-O-2 gas mixture) on the transparency and conductivity of the formed layers was investigated. The ITO films obtained both by RF and DC magnetron sputtering at room temperature have a high transparency in the visible wavelength range (80-85%) and a low surface resistance (20-25 Omega/sq for similar to 300 nm thickness) but their optimized deposition conditions and structural properties are significantly different. The DC sputtering can be performed in pure Ar with a lower discharge power density (1.0 W/cm(2)) and relatively high deposition rate (similar to 60 nm/min) while the RF sputtering requires Ar-O-2 (3.0 vol.% O-2) gas mixture, higher discharge power density (1.5 W/cm(2)) and yields a lower deposition rate (similar to 20 nm/mm). The RF sputtered ITO layers show a crystalline structure with strong (2 2 2), (4 0 0), (4 4 0), (6 2 2) X-ray diffraction peak intensities while the DC layers are amorphous with surface morphology formed by nano-scale grains. (c) 2006 Elsevier B.V. All rights reserved.
引用
收藏
页码:1466 / 1470
页数:5
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