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High performance enhancement-mode HEMT with 3DEG to conduct current and 3DHG as back barrier

机译:高性能增强模式HEMT,带有3DEG来传导电流,而3DHG作为背栅

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A novel enhancement-mode (E-mode) high electron mobility transistor (HEMT) with three-dimensional electron gas (3DEG) and three-dimensional hole gas (3DHG) is presented. It features a GaN-top layer, a positive graded AlGaN barrier layer (GAL), and a negative graded AlGaN back barrier layer (GABL) (wherein the positiveegative doping gradient is defined with respect to the growth direction), with a vertical conduction channel aside a MIS trench gate. The 2DHG is formed at the interface between the GaN-top layer and GAL. The 3DEG and 3DHG are formed due to the polarization induced by linearly grading Aluminum (Al) composition from 0 to x_(Al) in GAL and 0.4 to 0 in GABL, respectively. The source and drain locate at the same side of the MIS trench gate, and the source contacts with the gate. Firstly, 2DHG blocks the electron current conduction path between the source and 3DEG so as to achieve E-mode. Secondly, the high-sheet density 3DEG in GAL greatly increases the on-state current. Thirdly, the leakage current effectively is reduced by the 3DHG in GABL, improving the breakdown voltage. Fourthly, a high breakdown voltage (BV) is obtained because the polarization junction formed by the polarization charges in GAL and GABL improves the electric field distribution in the drift region. The BV of the proposed HEMT increases to 1080 V from 47 V of the conventional MIS HEMT at the same length of the drift region, and specific on-resistance (R_(on,sp)) decreases to 0.29 mΩ cm~2 from 0.64mΩcm~2 in simulation.
机译:提出了一种具有三维电子气(3DEG)和三维空穴气(3DHG)的新型增强模式(E模式)高电子迁移率晶体管(HEMT)。它具有GaN顶层,正梯度AlGaN势垒层(GAL)和负梯度AlGaN背势垒层(GABL)(其中,相对于生长方向定义了正/负掺杂梯度),并且垂直传导沟道放在MIS沟槽栅极旁。在GaN顶层和GAL之间的界面处形成2DHG。 3DEG和3DHG的形成是由于分别对GAL中的铝(Al)组成从0到x_(Al)和0.4至0的线性线性分级所引起的极化而形成的。源极和漏极位于MIS沟槽栅极的同一侧,并且源极与栅极接触。首先,2DHG阻断了源极和3DEG之间的电子电流传导路径,从而实现了E模式。其次,GAL中的高薄片密度3DEG大大增加了导通电流。第三,GABL中的3DHG有效降低了漏电流,提高了击穿电压。第四,由于由GAL和GABL中的极化电荷形成的极化结改善了漂移区中的电场分布,因此获得了高击穿电压(BV)。提出的HEMT的BV在相同的漂移区长度下从常规MIS HEMT的47 V增加到1080 V,比导通电阻(R_(on,sp))从0.64mΩcm减小到0.29mΩcm〜2在仿真中约为2。

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