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Raman and conductivity studies of boron-doped microcrystalline diamond, facetted nanocrystalline diamond and cauliflower diamond films

机译:掺硼微晶金刚石,多面纳米晶金刚石和花椰菜金刚石膜的拉曼和电导率研究

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We present a large amount of data showing how the electrical conductivity and Raman spectra of boron-doped CVD diamond films vary as a function of both B content and film type -- in particular, diamond crystallite size. Three types of film have been investigated: microcrystalline diamond (MCD), faceted nanocrystalline diamond (f-NCD) and 'cauliflower' diamond (c-NCD). For the same B content (measured by SIMS), the conductance of MCD films was much higher than those for the two types of smaller grained films. Multi-wavelength laser Raman spectroscopy showed that Fano interference effects were much reduced for the smaller grain-sized material. The position of the Lorentzian contribution to the 500 cm~(-1) Raman feature was used to estimate the B content in each type of film, and compared to the value measured using SIMS. We found that the Raman method overestimated the concentration of B by a factor of approx 5 for the f-NCD and c-NCD films, although it remains reasonably accurate for MCD films. The shortfall may be explained if only a small fraction of the B found in the small-grained films is being incorporated into substitutional sites. We conclude that in diamond films with a high concentration of grain boundaries, the majority of the B (80 percent in some cases) must be present at sites that do not contribute to the continuum of electronic states that give rise to metallic conductivity and the Fano effects. Such sites may include (a) interstitials, (b) the surface of the crystallites, or (c) bonded within the non-diamond carbon impurities present at the grain boundaries. This suggests that heavy doping of nanograined diamond films will give rise to a material with many different conducting regions, and possibly different conducting pathways and mechanisms.
机译:我们提供了大量数据,这些数据表明掺硼CVD金刚石膜的电导率和拉曼光谱如何随B含量和膜类型-特别是金刚石微晶尺寸的变化而变化。已经研究了三种类型的薄膜:微晶金刚石(MCD),多面纳米晶金刚石(f-NCD)和“花椰菜”金刚石(c-NCD)。对于相同的B含量(通过SIMS测量),MCD薄膜的电导率远远高于两种较小颗粒薄膜的电导率。多波长激光拉曼光谱表明,对于较小粒度的材料,Fano干涉效应大大降低。使用洛伦兹贡献对500 cm〜(-1)拉曼特征的贡献的位置来估计每种类型的胶片中的B含量,并将其与使用SIMS测量的值进行比较。我们发现,对于f-NCD和c-NCD膜,拉曼方法高估了B的浓度约5倍,尽管对于MCD膜仍保持相当准确。如果仅将小颗粒薄膜中发现的B的一小部分掺入替代位点,则可以解释这种不足。我们得出的结论是,在具有高晶界浓度的金刚石薄膜中,大多数B(某些情况下为80%)必须存在于无助于产生金属导电性和Fano的连续电子态的位置效果。这样的位点可以包括(a)间隙,(b)微晶的表面,或(c)结合在存在于晶界处的非金刚石碳杂质内。这表明对纳米颗粒金刚石薄膜进行重掺杂将产生一种具有许多不同导电区域,可能具有不同导电路径和机理的材料。

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