†Department of Engineering Physics, Polytechnique Montréal, C. P. 6079, Succ. Centre-Ville, Montréal, Québec H3C 3A7, Canada.
‡Max Planck Institute of Microstructure Physics, Weinberg 2, D 06120 Halle (Saale), Germany.
Nano Lett. 2015 Jun 10;15(6):3885-93. doi: 10.1021/acs.nanolett.5b00708. Epub 2015 May 29.
The introduction of stable isotopes in the fabrication of semiconductor nanowires provides an additional degree of freedom to manipulate their basic properties, design an entirely new class of devices, and highlight subtle but important nanoscale and quantum phenomena. With this perspective, we report on phonon engineering in metal-catalyzed silicon nanowires with tailor-made isotopic compositions grown using isotopically enriched silane precursors (28)SiH4, (29)SiH4, and (30)SiH4 with purity better than 99.9%. More specifically, isotopically mixed nanowires (28)Si(x)(30)Si(1-x) with a composition close to the highest mass disorder (x ∼ 0.5) were investigated. The effect of mass disorder on the phonon behavior was elucidated and compared to that in isotopically pure (29)Si nanowires having a similar reduced mass. We found that the disorder-induced enhancement in phonon scattering in isotopically mixed nanowires is unexpectedly much more significant than in bulk crystals of close isotopic compositions. This effect is explained by a nonuniform distribution of (28)Si and (30)Si isotopes in the grown isotopically mixed nanowires with local compositions ranging from x = ∼0.25 to 0.70. Moreover, we also observed that upon heating, phonons in (28)Si(x)(30)Si(1-x) nanowires behave remarkably differently from those in (29)Si nanowires suggesting a reduced thermal conductivity induced by mass disorder. Using Raman nanothermometry, we found that the thermal conductivity of isotopically mixed (28)Si(x)(30)Si(1-x) nanowires is ∼30% lower than that of isotopically pure (29)Si nanowires in agreement with theoretical predictions.
在半导体纳米线的制造中引入稳定同位素为操纵其基本性质、设计全新类别的器件以及突出微妙但重要的纳米级和量子现象提供了额外的自由度。基于这一观点,我们报告了使用同位素丰度大于 99.9%的同位素富集硅烷前体 (28)SiH4、(29)SiH4 和 (30)SiH4 生长的金属催化硅纳米线中的声子工程。更具体地说,研究了组成接近最高质量无序 (x ∼ 0.5) 的同位素混合纳米线 (28)Si(x)(30)Si(1-x)。阐明了质量无序对声子行为的影响,并将其与具有相似约化质量的同位素纯 (29)Si 纳米线进行了比较。我们发现,在同位素混合纳米线中,无序诱导的声子散射增强比具有相近同位素组成的体晶体中的增强要显著得多。这种效应可以通过生长的同位素混合纳米线中 (28)Si 和 (30)Si 同位素的不均匀分布来解释,其局部组成范围从 x = ∼0.25 到 0.70。此外,我们还观察到,在加热时,(28)Si(x)(30)Si(1-x)纳米线中的声子表现出与 (29)Si 纳米线明显不同的行为,这表明质量无序导致热导率降低。通过 Raman 纳米热测量法,我们发现同位素混合 (28)Si(x)(30)Si(1-x)纳米线的热导率比同位素纯 (29)Si 纳米线低约 30%,这与理论预测一致。