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Deep Traps in AlGaN/GaN Heterostructures Studied by Deep Level Transient Spectroscopy: Effect of Carbon Concentration in GaN Buffer Layers

机译:深能级瞬态光谱研究AlGaN / GaN异质结构中的深陷阱:GaN缓冲层中碳浓度的影响

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摘要

Electrical properties, including leakage currents, threshold voltages, and deep traps, of AlGaN/GaN heterostructure wafers with different concentrations of carbon in the GaN buffer layer, have been investigated by temperature dependent current-voltage and capacitance-voltage measurements and deep level transient spectroscopy (DLTS), using Schottky barrier diodes (SBDs). It is found that (i) SBDs fabricated on the wafers with GaN buffer layers containing a low concentration of carbon (low-[C] SBD) or a high concentration of carbon (high-[C] SBD) have similar low leakage currents even at 500 K; and (ii) the low-[C] SBD exhibits a larger (negative) threshold voltage than the high-[C] SBD. Detailed DLTS measurements on the two SBDs show that (i) different trap species are seen in the two SBDs: electron traps Ax (0.9 eV), A1 (0.99 eV), and A2 (1.2 eV), and a holelike trap H1 (1.24 eV) in the low-[C] SBD; and electron traps A1, A2, and A3 ( ∼ 1.3 eV), and a holelike trap H2 (\u3e1.3 eV) in the high-[C] SBD; (ii) for both SDBs, in the region close to GaN buffer layer, only electron traps can be detected, while in the AlGaN/GaN interface region, significant holelike traps appear; and iii) all of the deep traps show a strong dependence of the DLTS signal on filling pulse width, which indicates they are associated with extended defects, such as threading dislocations. However, the overall density of electron traps is lower in the low-[C] SBD than in the high-[C] SBD. The different traps observed in the two SBDs are thought to be mainly related to differences in microstructure (grain size and threading dislocation density) of GaN buffer layers grown at different pressures.
机译:已通过与温度相关的电流-电压和电容-电压测量以及深能级瞬态光谱法研究了GaN缓冲层中碳浓度不同的AlGaN / GaN异质结构晶圆的电性能,包括泄漏电流,阈值电压和深陷阱(DLTS),使用肖特基势垒二极管(SBD)。发现(i)在具有GaN缓冲层的晶圆上制造的SBD含有低浓度的碳(low- [C] SBD)或高浓度的碳(high- [C] SBD)甚至具有相似的低漏电流在500 K; (ii)低[C] SBD的阈值电压比高[C] SBD的阈值电压大。在两个SBD上进行的详细DLTS测量表明(i)在两个SBD中看到了不同的陷阱种类:电子陷阱Ax(0.9 eV),A1(0.99 eV)和A2(1.2 eV),以及孔状陷阱H1(1.24) eV)在低[C] SBD中;高[C] SBD中的电子陷阱A1,A2和A3(约1.3 eV)和空穴状陷阱H2(\ u3e1.3 eV); (ii)对于两个SDB,在靠近GaN缓冲层的区域中,只能检测到电子陷阱,而在AlGaN / GaN界面区域中,会出现大量的空穴状陷阱; iii)所有的深陷阱都显示DLTS信号对填充脉冲宽度的强烈依赖性,这表明它们与扩展的缺陷(例如螺纹位错)有关。但是,低[C] SBD的电子陷阱的总密度低于高[C] SBD的电子陷阱的总密度。在两个SBD中观察到的不同陷阱被认为主要与在不同压力下生长的GaN缓冲层的微观结构(晶粒尺寸和螺纹位错密度)不同有关。

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