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首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >Engineering of electric field distribution in GaN(cap)/AlGaN/GaN heterostructures: theoretical and experimental studies
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Engineering of electric field distribution in GaN(cap)/AlGaN/GaN heterostructures: theoretical and experimental studies

机译:GaN(cap)/ AlGaN / GaN异质结构中的电场分布工程:理论和实验研究

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Polarization engineering of GaN-based heterostructures opens a way to develop advanced transistor heterostructures, although measurement of the electric field in such heterostructures is not a simple task. In this work, contactless electroreflectance (CER) spectroscopy has been applied to measure the electric field in GaN-based heterostructures. For a set of GaN(d = 0, 5, 15, and 30 nm)/AlGaN(20 nm)/GaN(buffer) heterostructures a decrease of electric field in the GaN(cap) layer from 0.66 MV cm(-1) to 0.27 MV cm(-1) and an increase of the electric field in the AlGaN layer from 0.57 MV cm(-1) to 0.99 MV cm(-1) have been observed with the increase in the GaN(cap) thickness from 5-30 nm. For a set of GaN(20 nm)/AlGaN(d = 10, 20, 30, and 40 nm)/GaN(buffer) heterostructures a decrease of the electric field in the AlGaN layer from 1.77 MV cm(-1) to 0.64 MV cm(-1) and an increase of the electric field in the GaN layer from 0.57 MV cm(-1) to 0.99 MV cm(-1) were observed with the increase in the AlGaN thickness from 10-40 nm. To determine the distribution of the electric field in these heterostructures the Schrodinger and Poisson equations are solved in a self-consistent manner and matched with experimental data. It is shown that the built-in electric field in the GaN(cap) and AlGaN layers obtained from measurements does not reach values of electric field resulting only from polarization effects. The measured electric fields are smaller due to a screening of polarization effects by free carriers, which are inhomogeneously distributed across the heterostructure and accumulate at interfaces. The results clearly demonstrate that CER measurements supported by theoretical calculations are able to determine the electric field distribution in GaN-based heterostructures quantitatively, which is very important for polarization engineering in this material system.
机译:GaN基异质结构的极化工程为开发先进的晶体管异质结构开辟了道路,尽管测量此类异质结构中的电场并非易事。在这项工作中,非接触电反射(CER)光谱已应用于测量GaN基异质结构中的电场。对于一组GaN(d = 0、5、15和30 nm)/ AlGaN(20 nm)/ GaN(缓冲)异质结构,GaN(帽)层中的电场从0.66 MV cm(-1)减少到0.27 MV cm(-1),随着GaN(帽)厚度从5的增加,观察到AlGaN层中的电场从0.57 MV cm(-1)增加到0.99 MV cm(-1)。 -30 nm。对于一组GaN(20 nm)/ AlGaN(d = 10、20、30和40 nm)/ GaN(缓冲)异质结构,AlGaN层中的电场从1.77 MV cm(-1)减小到0.64随着AlGaN厚度从10-40 nm的增加,观察到MV cm(-1)和GaN层中电场从0.57 MV cm(-1)增加到0.99 MV cm(-1)。为了确定这些异质结构中的电场分布,以自洽的方式求解了Schrodinger和Poisson方程,并与实验数据进行了匹配。结果表明,通过测量获得的GaN(cap)和AlGaN层中的内置电场不会达到仅由极化效应引起的电场值。由于自由载流子对极化效应的屏蔽,所测得的电场较小,自由载流子不均匀地分布在异质结构上并聚集在界面上。结果清楚地表明,理论计算支持的CER测量能够定量确定GaN基异质结构中的电场分布,这对于该材料系统中的极化工程非常重要。

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