纳米晶格错配异质结构的临界厚度

P. Lu, S.M. Wang
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引用次数: 0

摘要

近年来,纳米外延技术引起了人们的广泛关注。理论研究可以追溯到二十多年前,Luryi和Suhir (LS)研究了在脊状带上生长的应变外延层的临界厚度(Luryi, 1986)。他们使用了应变的解析表达式,并预测当条带宽度足够小(在nm范围内)时,临界厚度会增加到无穷大。Zubia和Hersee (ZH)采用同样的方法,考虑了在柔顺的图案衬底上生长的应变层,得到了相同的结论(Zubia, 1999)。在这两项研究中,当应变能超过位错能时定义临界厚度。然而,大量的实验表明,错配位错不能完全适应晶格错配,残余应变在临界厚度处并不趋于零。此外,Van Mieghem等人利用有限元法(FEM)研究了平行六面体应变层中的应变和应力,发现应变解析公式存在缺陷(Van Mieghem, 1994)。在这项工作中,我们研究了应变分布和临界厚度的应变层生长在纳米尺度的图案柔性基板上。我们考虑了残余应变分布,并表明预测的临界厚度比LS模型的预测值大得多。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Critical Thickness of Nano-scale Lattice Mismatched Heterostructures
Nano-epitaxy has attracted great attention in the last several years. Theoretical study can date back to more than twenty years ago when Luryi and Suhir (LS) studied critical thickness of a strained epi layer grown on a ridged strip (Luryi, 1986). They used an analytic expression for strain and predicted that the critical thickness increased to infinity when the strip width was small enough (in the nm range). Following the same approach, Zubia and Hersee (ZH) considered a strained layer grown on a compliant patterned substrate and got the same conclusion (Zubia, 1999). In both studies, a critical thickness is defined when the strain energy exceeds the dislocation energy. However, numerous experiments reveal that the lattice mismatch can not be completely accommodated by misfit dislocations and the residual strain does not go to zero at the critical thickness. In addition, Van Mieghem et al. investigated strain and stress in a parallelepiped strained layer using finite element method (FEM) and found that the analytic formula for strain was deficient (Van Mieghem, 1994). In this work, we investigate strain distribution and critical thickness of a strained layer grown on a nano-scale patterned compliant substrate using FEM. We take into account the residual strain distribution and show that the predicted critical thickness is much larger than those predicted values using the LS model.
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