2.3 kV 4H-SiC Accumulation-channel JBSFETs: Experimental Comparison of Linear, Hexagonal and Octagonal Cell Topologies

Aditi Agarwal, Kijeong Han, B. Baliga
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引用次数: 2

Abstract

The body diode of a SiC power MOSFET is not suitable for current conduction in the third quadrant due high on-state voltage drop, large reverse recovery losses [1] , and possibility of bipolar degradation [2] . Integrating a Junction Barrier Schottky (JBS) diode with the MOSFET (called JBSFET) solves these issues [3] , [4] for 1.2 kV devices. This paper reports experimental data on 2.3 kV JBSFETs with different cell topologies (Linear, Hexagonal and Octagonal) for the first time at this larger voltage capability .
2.3 kV 4H-SiC累积通道jbsfet:线性、六边形和八边形电池拓扑的实验比较
SiC功率MOSFET的主体二极管由于导通压降高、反向恢复损耗大[1]以及双极退化的可能性[2],不适合在第三象限传导电流。将结势垒肖特基(JBS)二极管与MOSFET集成(称为JBSFET)解决了1.2 kV器件的这些问题[3],[4]。本文首次报道了具有不同电池拓扑(线性、六边形和八边形)的2.3 kV jbsfet在这种较大电压能力下的实验数据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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