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克服低 Ge 离子化和侵蚀率变化,实现 Si(1-x)Ge(x)/Ge 量子阱结构的定量 ultralow 能量二次离子质谱深度剖面分析。

Overcoming low Ge ionization and erosion rate variation for quantitative ultralow energy secondary ion mass spectrometry depth profiles of Si(1-x)Ge(x)/Ge quantum well structures.

机构信息

Department of Physics, University of Warwick, Gibbet Hill Road, Coventry, CV4 7AL, UK.

出版信息

Anal Chem. 2012 Mar 6;84(5):2292-8. doi: 10.1021/ac202929x. Epub 2012 Feb 24.

Abstract

We specify the O(2)(+) probe conditions and subsequent data analysis required to obtain high depth resolution secondary ion mass spectrometry profiles from multiple Ge/Si(1-x)Ge(x) quantum well structures (0.6 ≤ x ≤ 1). Using an O(2)(+) beam at normal incidence and with energies >500 eV, we show that the measured Ge signal is not monotonic with concentration, the net result being an unrepresentative and unquantifiable depth profile. This behavior is attributed to a reduced Ge ionization rate as x approaches 1. At lower beam energies the signal behaves monotonically with Ge fraction, indicating that the Ge atoms are now ionizing more readily for the whole range of x, enabling quantitative profiles to be obtained. To establish the depth scale a point-by-point approach based on previously determined erosion rates as a function of x is shown to produce quantum well thicknesses in excellent agreement with those obtained using transmission electron microscopy. The findings presented here demonstrate that to obtain reliable quantitative depth profiles from Ge containing samples requires O(2)(+) ions below 500 eV and correct account to be taken of the erosion rate variation that exists between layers of different matrix composition.

摘要

我们指定了 O(2)(+)探针条件和后续数据分析要求,以从多个 Ge/Si(1-x)Ge(x)量子阱结构(0.6 ≤ x ≤ 1)中获得高深度分辨率二次离子质谱剖面。使用正常入射的 O(2)(+)束和能量>500 eV,我们表明测量的 Ge 信号与浓度不是单调的,净结果是一个不具代表性和不可量化的深度剖面。这种行为归因于 x 接近 1 时 Ge 离子化率降低。在较低的束能量下,信号随 Ge 分数单调变化,表明现在 Ge 原子在整个 x 范围内更容易离子化,从而能够获得定量剖面。为了建立深度标度,我们展示了一种基于先前确定的作为 x 的函数的侵蚀率的逐点方法,该方法产生的量子阱厚度与使用透射电子显微镜获得的厚度非常吻合。这里提出的发现表明,要从含 Ge 的样品中获得可靠的定量深度剖面,需要低于 500 eV 的 O(2)(+)离子,并正确考虑不同基质组成层之间存在的侵蚀率变化。

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