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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Germanium-induced texture and preferential orientation of NiSi_(1-x)Ge_x layers on Si_(1-x)Ge_x
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Germanium-induced texture and preferential orientation of NiSi_(1-x)Ge_x layers on Si_(1-x)Ge_x

机译:锗诱导的Si_(1-x)Ge_x上NiSi_(1-x)Ge_x层的织构和优先取向

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摘要

NiSi_(1-x)Ge_x films on compressively strained as well as relaxed undoped Si_(1-x)Ge_x epitaxially grown substrates with x=0.06-0.30 on Si(001) wafers have been studied with respect to the relative orientation of film and substrate after annealing at temperatures in the range 400-850℃. Using x-ray diffraction, transmission electron microscopy, and pole-figure measurements, it was found that only the monogermanosilicide phase formed above 450℃ and was the only phase still at 850℃. New information regarding the effects of Ge on the silicidation of Ni was also found. Thus, the preferred plane parallel to the surface is (013). Compared to NiSi, Ge suppresses the development of the other planes parallel to the surface except (013). Within this plane, the orientations of the grains pile up in such a way that the configuration NiSi_(1-x)Ge_x[100]//Si_(1-x)Ge_x[100] is avoided, which in the pole-figures leads to broad peaks in-between the substrate [100] and [010]. In addition, peaks indicating the epitaxial alignment NiSi_(0.8)Ge_(0.2)(±21-1) or (±2-11)//Si_(0.8)Ge_(0.2)(±2±20) coupled with NiSi_(0.8)Ge_(0.2)(±100) ≈ //Si_(0.8)Ge_(0.2)(±100) or (0±10) were found. Fine structure in the broad peaks is found to be due to lateral epitaxial alignments between grains along their common grain boundary. Based on the nonex- istence of NiGe_2, the observations are interpreted in terms of Ge preventing the formation of certain Ni-Ge bonds at the interface between NiSi_(1-x)Ge_x and the Si_(1-x)Ge_x substrate.
机译:研究了在Si(001)晶片上压缩应变以及松弛x = 0.06-0.30的未掺杂Si_(1-x)Ge_x外延生长衬底上的NiSi_(1-x)Ge_x膜的相对取向和在400-850℃的温度范围内退火后的衬底。通过X射线衍射,透射电子显微镜和极图测量,发现在450℃以上仅形成单锗硅化物相,而在850℃仍是唯一的相。还发现了有关Ge对Ni的硅化作用的新信息。因此,平行于表面的优选平面是(013)。与NiSi相比,Ge抑制了除了(013)以外与表面平行的其他平面的发展。在该平面内,晶粒的方向堆积成使得避免配置NiSi_(1-x)Ge_x [100] // Si_(1-x)Ge_x [100],这在极坐标图中会导致在底物[100]和[010]之间的宽峰。另外,表示与NiSi_(0.8)耦合的外延取向NiSi_(0.8)Ge_(0.2)(±21-1)或(±2-11)// Si_(0.8)Ge_(0.2)(±2±20)的峰)Ge_(0.2)(±100)≈//Si_(0.8)Ge_(0.2)(±100)或(0±10)。发现宽峰中的精细结构归因于晶粒之间沿其共同晶粒边界的横向外延排列。基于NiGe_2的不存在,可以用Ge来解释观察结果,以防止在NiSi_(1-x)Ge_x和Si_(1-x)Ge_x衬底之间的界面处形成某些Ni-Ge键。

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