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High-fluence ion implantation of In into Al crystals: formation and evolution of buried layers

机译:In高效离子注入Al晶体:埋层的形成与演化

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Al(110) single-crystal samples were implanted at T = 200 degrees C with In+ ions of 250 keV energy with fluences ranging from 4 x 10(20) to 3 x 10(21)m(-2). The implantation resulted in the formation of In precipitates growing with fluence in topotactical alignment with the host matrix. High-fluence implantation was used in an attempt to produce single-crystal buried layers of In embedded into Al. Rutherford back-scattering (RBS)-channelling analysis of the implanted samples and transmission electron microscopy studies of the incorporated In layer morphology were carried out. With increasing fluence the peak In concentration was observed to increase gradually until a maximum value of (a)bout 38 at.% was reached at an implantation dose of 1.5 x 10(21) m(-2). The buried layer thus formed was found to have fragmentary morphology consisting os large In precipitates. During further implantation the peak concentration decreased drastically to reach a steady state; In order to study a possible effect of sputtering on the In profile evolution, sputtered atoms were collected in situ on carbon foils during implantation. The foils were subsequently analysed by RES analysis to determine the partial sputtering yields for In and Al independently. Both partial sputtering yields were found to change with fluence. The evolution of the In depth distribution profile showed that the high peak concentrations are achieved as a result of competition between the diffusion of the implanted indium and matrix surface erosion due to sputtering. [References: 30]
机译:Al(110)单晶样品在T = 200摄氏度下注入250 keV能量的In +离子,注量范围为4 x 10(20)到3 x 10(21)m(-2)。注入导致形成In沉淀物,该沉淀物随着与主体基质的定势排列的影响而生长。使用高通量注入来尝试产生嵌入到Al中的In的单晶埋层。进行了Rutherford背散射(RBS)通道注入样品的分析和掺入In层形态的透射电子显微镜研究。随着注量的增加,观察到In浓度峰值逐渐增加,直到在1.5 x 10(21)m(-2)的注入剂量下达到38 a.bout的最大值。发现由此形成的掩埋层具有由大的In沉淀物组成的碎片形态。在进一步的植入过程中,峰值浓度急剧下降,达到了稳态。为了研究溅射对In轮廓演变的可能影响,在注入过程中将溅射的原子原位收集在碳箔上。随后通过RES分析对箔进行分析,以独立地确定In和Al的部分溅射产率。发现两种部分溅射产量都随着注量而变化。 In深度分布曲线的演变表明,由于注入的铟的扩散与溅射引起的基体表面腐蚀之间的竞争,获得了较高的峰浓度。 [参考:30]

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