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Electron scattering mechanisms in GZO films grown on a-sapphire substrates by plasma-enhanced molecular beam epitaxy

机译:等离子体增强分子束外延在a-蓝宝石衬底上生长的GZO膜中的电子散射机理

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摘要

We report on the mechanisms governing electron transport using a comprehensive set of ZnO layers heavily doped with Ga (GZO) grown by plasma-enhanced molecular-beam epitaxy on a-plane sapphire substrates with varying oxygen-to-metal ratios and Ga fluxes. The analyses were conducted by temperature dependent Hall measurements which were supported by microstructural investigations as well. Highly degenerate GZO layers with n > 5 × 1020 cm-3 grown under metal-rich conditions (reactive oxygen-to-metal ratio <1) show relatively larger grains (∼20–25 nm by x-ray diffraction) with low-angle boundaries parallel to the polar c-direction. For highly conductive GZO layers, ionized-impurity scattering with almost no compensation is the dominant mechanism limiting the mobility in the temperature range from 15 to 330 K and the grain-boundary scattering governed by quantum-mechanical tunnelling is negligible. However, due to the polar nature of ZnO having high crystalline quality, polar optical phonon scattering cannot be neglected for temperatures above 150 K, because it further reduces mobility although its effect is still substantially weaker than the ionized impurity scattering even at room temperature (RT). Analysis of transport measurements and sample microstructures by x-ray diffraction and transmission electron microscopy led to a correlation between the grain sizes in these layers and mobility even for samples with a carrier concentration in the upper 1020 cm-3 range. In contrast, electron transport in GZO layers grown under oxygen-rich conditions (reactive oxygen-to-metal ratio >1), which have inclined grain boundaries and relatively smaller grain sizes of 10–20 nm by x-ray diffraction, is mainly limited by compensation caused by acceptor-type point-defect complexes, presumably (GaZn-VZn), and sca- tering on grain boundaries. The GZO layers with n <1020 cm-3 grown under metal-rich conditions with reduced Ga fluxes show a clear signature of grain-boundary scattering governed by the thermionic effect in the temperature-dependent mobility but with much higher RT mobility values compared to the samples grown under oxygen-rich conditions [34 vs. 7.5 cm2/V·s]. Properties of GZO layers grown under different conditions clearly indicate that to achieve highly conductive GZO, metal-rich conditions instead of oxygen-rich conditions have to be used.
机译:我们报告了使用一系列由重掺杂Ga(GZO)重掺杂的ZnO层控制电子传输的机制,该ZnO层是通过等离子蓝宝石衬底上具有不同的氧金属比和Ga通量的等离子体增强分子束外延生长的。分析通过与温度相关的霍尔测量进行,该测量也得到微观结构研究的支持。在富金属条件下(活性氧与金属的比<1)生长的n> 5×10 20 cm -3 的高度退化的GZO层显示出相对较大的晶粒( X射线衍射约20-25nm),低角度边界平行于极性c方向。对于高导电性的GZO层,几乎没有补偿的离子杂质扩散是限制在15至330 K温度范围内迁移率的主要机理,而由量子机械隧穿控制的晶界散射可以忽略不计。然而,由于具有高结晶质量的ZnO的极性,在150 K以上的温度下不能忽略极性光子声子散射,因为即使在室温下,它的作用仍远比电离杂质散射弱,尽管它的作用仍大大弱于电离杂质散射。 )。通过X射线衍射和透射电子显微镜对传输测量和样品微观结构的分析导致这些层的晶粒尺寸与迁移率之间存在相关性,即使对于载流子浓度在10 20 cm < sup> -3 范围。相反,主要限制了在富氧条件(反应性氧与金属之比> 1)下生长的GZO层中的电子传输,该层具有倾斜的晶界和相对较小的晶粒尺寸(通过X射线衍射)为10-20 nm。通过由受体型点缺陷复合物(大概是(GaZn-VZn))引起的补偿,并在晶界上散布。在富金属条件下生长的n <10 20 cm -3 的GZO层具有减少的Ga通量,显示出受热离子作用控制的晶界散射的清晰特征。与在富氧条件下生长的样品相比,温度依赖性迁移率具有更高的RT迁移率值[34 vs. 7.5 cm 2 / V·s]。在不同条件下生长的GZO层的特性清楚地表明,要实现高导电性的GZO,必须使用富金属条件而不是富氧条件。

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  • 来源
    《Journal of Applied Physics》 |2012年第10期|p.1-9|共9页
  • 作者

    Liu H. Y.;

  • 作者单位
  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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