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氮化镓/铝镓氮异质结构的原子探针:电场、样品晶体学和激光激发在定量分析中的作用

Atom probe of GaN/AlGaN heterostructures: The role of electric field, sample crystallography and laser excitation on quantification.

作者信息

Morris Richard J H, Cuduvally Ramya, Melkonyan Davit, Zhao Ming, van der Heide Paul, Vandervorst Wilfried

机构信息

IMEC, Kapeldreef 75, 3001, Leuven, Belgium.

IMEC, Kapeldreef 75, 3001, Leuven, Belgium; Instituut voor Kern- en Stralingsfysica, KU Leuven, Leuven, Belgium.

出版信息

Ultramicroscopy. 2019 Nov;206:112813. doi: 10.1016/j.ultramic.2019.112813. Epub 2019 Jul 8.

Abstract

Scaling and non-planar architectures are key factors helping to advance the semiconductor field. Accurate 3-dimensional atomic scale information is therefore sought but this presents a significant metrology challenge. Atom probe tomography has emerged as a strong candidate to fulfill this role, but before it can be considered an accurate and precise metrology method, numerous difficulties need to be overcome. In this paper we highlight some of these in respect to the analysis of GaN/AlGaN device heterostructures. Although a significant range of conditions for accurate GaN stoichiometric analysis were readily achieved, a more limited range of analysis conditions that yielded an accurate Al site fraction for AlGaN was observed because the Al was typically overestimated. Moreover, the low index planes of the material resulted in pole and zone lines given their lower evaporation fields and are clearly observed on the detector due to related ion trajectory aberrations representative of local field variations present. As a result of the strong compositional bias of GaN analysis with field, the Ga and N concentrations were found to vary by ∼20 at.% over the tip apex. For the AlGaN this variation was smaller (<4 at.%), even for a similar magnitude of tip field variation.

摘要

缩放和非平面架构是推动半导体领域发展的关键因素。因此,人们追求精确的三维原子尺度信息,但这带来了重大的计量挑战。原子探针断层扫描已成为履行这一职责的有力候选方法,但在它被视为一种准确且精确的计量方法之前,需要克服诸多困难。在本文中,我们针对氮化镓/氮化铝镓器件异质结构的分析突出了其中一些困难。尽管很容易实现一系列用于精确氮化镓化学计量分析的条件,但观察到能得出准确的氮化铝镓铝位点分数的分析条件范围较为有限,因为铝通常被高估。此外,材料的低指数平面因其较低的蒸发场导致极线和区线出现,并且由于代表局部场变化的相关离子轨迹像差,在探测器上能清晰观察到这些极线和区线。由于氮化镓分析中成分随场强有强烈偏差,发现在针尖顶端,镓和氮的浓度变化约20原子百分比。对于氮化铝镓,即使针尖场强变化幅度相似,这种变化也较小(<4原子百分比)。

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