Structure zone model for extreme shadowing conditions

被引:99
作者
Mukherjee, S. [1 ]
Gall, D. [1 ]
机构
[1] Rensselaer Polytech Inst, Dept Mat Sci & Engn, Troy, NY 12180 USA
基金
美国国家科学基金会;
关键词
Structure zone model; Physical vapor deposition; Glancing angle deposition; Atomic shadowing; Surface diffusion; Whisker; GLANCING ANGLE DEPOSITION; THIN-FILM; SUBSTRATE-TEMPERATURE; TA NANOPILLARS; GROWTH; ARRAYS;
D O I
10.1016/j.tsf.2012.11.007
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Previously reported data on the microstructure of glancing angle deposited (GLAD) metal layers is used to extend the qualitative arguments of the structure zone model for physical vapor deposition to growth conditions with exacerbated atomic shadowing. At low growth temperatures T-s relative to the melting point T-m, the microstructural development is governed by atomic shadowing for both normal deposition and GLAD, resulting in fibrous grains with voided boundaries (Zone I). As the homologous growth temperature theta = T-s/T-m is raised above approximately 0.3, GLAD layers continue to exhibit well separated columns while conventional thin films show dense columnar microstructures (Zone II). theta>0.5 leads to equiaxed grains independent of deposition angle (Zone III). Therefore, strong shadowing during GLAD suppresses Zone II microstructures, causing a direct transition from Zone I to Zone III. GLAD microstructures can be divided into four distinct zones: rods, columns, protrusions, and equiaxed grains: separated self-affine rods form for theta <theta(c) = 0.24 +/- 0.2, while considerably broader columns develop at theta>theta(c), due to exacerbated self-shadowing associated with an increased growth front roughness, causing larger growth exponents. Above theta approximate to 0.35, protrusions develop on top of some columns as they capture an overproportionate amount of deposition flux and grow much higher than the surrounding layer. At theta>0.5, diffusion processes dominate over atomic shadowing, leading to faceted rough layers with equiaxed grains. In addition, the large mass transport facilitates the formation of whiskers that form for many metal GLAD layers at theta>0.4. (C) 2012 Elsevier B.V. All rights reserved.
引用
收藏
页码:158 / 163
页数:6
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