This paper compares and evaluates the single pulse short-circuit robustness of SiC MOSFETs with linear and hexagonal cell topologies under different gate voltages, bus voltages, and case temperatures. The short-circuit failure mechanisms of the linear and hexagonal cell topologies are studied. A new switching model for gate failure and thermal runaway short-circuit failure modes is proposed and analyzed. The robustness performance of the linear and hexagonal cell topologies is compared and evaluated under the same short-circuit power for the first time, fully revealing the comprehensive impact mechanism of cell topologies on the short-circuit robustness for SiC MOSFETs.@en

With the increase in voltage level and current capacity of the insulated gate bipolar transistor (IGBT), the avalanche effect has become an important factor limiting the safe operating area (SOA) of the device. The hole injection into the p/n junction on the backside of the IGBT after avalanche is the main feature that distinguishes the avalanche effect from other devices. In this paper, the avalanche breakdown characteristics of IGBT and the nature of current filament are investigated using theoretical analysis and numerical simulation, and the underlying physical mechanism controlling the nature of current filaments is revealed. The results show that the hole injection on the backside of the IGBT leads to an additional negative differential resistance (NDR) branch on the avalanche breakdown curve. The device’s common-base current gain, αpnp, is a crucial factor in determining the current filament. As αpnp increases, the avalanche-induced current filament becomes stronger and slower, resulting in weaker avalanche robustness of the device.@en

Two P-Based depth of SiC VDMOSFETs (group A and B) are designed and manufactured by enhanced P-Based implantation. The group A with lower P-based depth has a better static properties, while group B has a higher high frequency switching performance. Further, the avalanche reliability and failure mechanism for two groups are investigated by UIS experiment and TCAD simulation. The results show that the high temperature is generated by energy dissipation during avalanche and it drives the parasitic BJT conduction, causing Ids out of control and instantaneous heat concentration in a very short time. Significantly, high P-Based depth exhibits higher UIS reliability due to smaller Rb and more difficult to active parasitic BJT.@en

A novel 4H-SiC Multiple Stepped SGT MOSFET (MSGT-MOSFET) is presented and investigated utilizing TCAD simulations in this paper. We have quantitatively studied the characteristics of the device through simulation modeling and physical model calculations, and comparatively analyzed the performance and application prospects of this novel device. The gate-to-drain capacitance (C_gd) and gate-to-drain charge (Q_gd) of the MSGT-MOSFET are significantly reduced in comparison with the double trench MOSFET (DT-MOSFET) and the conventional SGT MOSFET (CSGT-MOSFET), due to the reduction of the overlapping area of the split gate (SG) structure and drift region. Therefore, the obtained high frequency figure of merit (HF-FOM) defined as [R_on × C_gd] reduced by 23.9% compared with DT-MOSFET and CSGT-MOSFET. And the HF-FOM [R_on × Q_gd] for the MSGT-MOSFET significantly decreased by 71% and 50%, respectively, compared to that of the DT-MOSFET and CSGT-MOSFET. Furthermore, the switching loss is also simulated and calculated. And the total switching loss of the proposed MSGT-MOSFET realizes 42.9% and 21.7% reduction in comparison with the DT-MOSFET and CSGT-MOSFET. The overall enhanced performances suggest that the MSGT-MOSFET is an excellent choice for high frequency power electronic applications.

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To investigate the unclamped inductive switch (UIS) characteristics, 1200 V silicon carbide (SiC) planar MOSFETs with four cell topologies of linear, current sharing linear, square, and hexagon are designed and manufactured. The experimental platform was built and tested. The results show that the single pulse avalanche energy density of the linear cell topology is 1.69 times higher than that of the square and 1.49 times that of the hexagon. Further, the UIS process is simulated by using physical simulation, which shows that the avalanche energy was concentrated near the corner of the P-base region in the UIS mode. From this, the avalanche energy distribution differences of the four cell topologies were analyzed and compared. A theoretical model of avalanche heating per unit area is proposed, which shows that the avalanche energy density is inversely proportional to the proportion of avalanche energy concentration region. This study may contribute to the cell topology design of SiC MOSFETs under the application scenario with high avalanche reliability requirements.@en