Norouzpour Mana, Rakhsha Ramtin, Herring Rodney
CAMTEC, MENG, University of Victoria, British Colombia, Canada V8W 2Y2.
Micron. 2017 Jun;97:68-77. doi: 10.1016/j.micron.2017.02.010. Epub 2017 Mar 10.
A characteristic of the majority of semiconductors is the presence of lattice strain varying with the nanometer scale. Strain originates from the lattice mismatch between layers of different composition deposited during epitaxial growth. Strain can increase the mobility of the charge carriers by the band gap reduction. So, measuring atomic displacement inside crystals is an important field of interest in semiconductor industry. Among all available transmission electron microscopy techniques offering nano-scale resolution measurements, convergent beam electron diffraction (CBED) patterns show the highest sensitivity to the atomic displacement. Higher Order Laue Zone (HOLZ) lines split by small non-uniform variations of lattice constant allowing to measure the atomic displacement through the crystal. However, it could only reveal the atomic displacement in two dimensions, i.e., within the x-y plane of the thin film of TEM specimen. The z-axis atomic displacement which is along the path of the electron beam has been missing. This information can be obtained by recovering the phase information across the split HOLZ line using the self-interference of the split HOLZ line (SIS-HOLZ). In this work, we report the analytical approach used to attain the phase profile across the split HOLZ line. The phase profile is studied for three different atomic displacement fields in the Si substrate at 80nm away from its interface with Si/SiGe superlattices.
大多数半导体的一个特性是存在随纳米尺度变化的晶格应变。应变源于外延生长过程中沉积的不同成分层之间的晶格失配。应变可通过减小带隙来提高电荷载流子的迁移率。因此,测量晶体内部的原子位移是半导体行业一个重要的研究领域。在所有能够提供纳米级分辨率测量的透射电子显微镜技术中,会聚束电子衍射(CBED)图案对原子位移表现出最高的灵敏度。高阶劳厄区(HOLZ)线会因晶格常数的微小不均匀变化而分裂,从而能够测量穿过晶体的原子位移。然而,它只能揭示二维的原子位移,即在透射电镜样品薄膜的x - y平面内。沿电子束路径的z轴原子位移一直缺失。通过利用分裂HOLZ线的自干涉(SIS - HOLZ)恢复分裂HOLZ线的相位信息,可以获得此信息。在这项工作中,我们报告了用于获取分裂HOLZ线相位分布的分析方法。研究了在距其与Si/SiGe超晶格界面80nm处的Si衬底中三种不同原子位移场的相位分布。