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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Band-gap measurements of direct and indirect semiconductors using monochromated electrons
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Band-gap measurements of direct and indirect semiconductors using monochromated electrons

机译:使用单色电子对直接和间接半导体进行带隙测量

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With the development of monochromators for transmission electron microscopes, valence electron-energy-loss spectroscopy (VEELS) has become a powerful technique to study the band structure of materials with high spatial resolution. However, artifacts such as Cerenkov radiation pose a limit for interpretation of the low-loss spectra. In order to reveal the exact band-gap onset using the VEELS method, semiconductors with direct and indirect band-gap transitions have to be treated differently. For direct semiconductors, spectra acquired at thin regions can efficiently minimize the Cerenkov effects. Examples of hexagonal GaN (h-GaN) spectra acquired at different thickness showed that a correct band-gap onset value can be obtained for sample thicknesses up to 0.5 t/λ. In addition, ω-q maps acquired at different specimen thicknesses confirm the thickness dependency of Cerenkov losses. For indirect semiconductors, the correct band-gap onset can be obtained in the dark-field mode when the required momentum transfer for indirect transition is satisfied. Dark-field VEEL spectroscopy using a star-shaped entrance aperture provides a way of removing Cerenkov effects in diffraction mode. Examples of Si spectra acquired by displacing the objective aperture revealed the exact indirect transition gap E_g of 1.1 eV.
机译:随着用于透射电子显微镜的单色仪的发展,价电子能量损失谱(VEELS)已成为研究具有高空间分辨率的材料的能带结构的强大技术。但是,诸如切伦科夫辐射的伪影为解释低损耗光谱带来了限制。为了使用VEELS方法揭示确切的带隙起始点,必须对具有直接和间接带隙跃迁的半导体进行不同的处理。对于直接半导体,在薄区域获取的光谱可以有效地最小化切伦科夫效应。在不同厚度下获取的六方氮化镓(h-GaN)光谱的示例表明,对于不超过0.5 t /λ的样品厚度,可以获得正确的带隙起始值。另外,在不同样品厚度下获得的ω-q图证实了切伦科夫损失的厚度依赖性。对于间接半导体,当满足间接过渡所需的动量传递时,可以在暗场模式下获得正确的带隙起始。使用星形入射孔的暗场VEEL光谱学提供了一种在衍射模式下消除切伦科夫效应的方法。通过移动物镜孔径获得的Si光谱示例显示,确切的间接跃迁间隙E_g为1.1 eV。

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