This paper reports on a 400 watt boost converter using a SiC BJT and a SiC MOSFET as the switch and a 6 Amp and a 50 Amp SiC Schottky diode as the output rectifier. The converter was operated at 100 kHz with an input voltage of 200 volts DC and an output voltage of 400 volts DC. The efficiency was tested with an output loaded from 50 watts to 400 watts at baseplate temperatures of 25°C, 100°C, 150°C and 200°C. The results show the converter in all cases capable of operating at temperatures beyond the range possible with silicon power devices. While the converter efficiency was excellent in all cases, the SiC MOSFET and 6 Amp Schottky diode had the highest efficiency. Since the losses in a boost converter are dominated by the switching losses and the switching losses of the SiC devices are unaffected by temperature, the efficiency of the converter was effectively unchanged as a function of temperature.
This paper presents the development of 1000 V, 30A bipolar junction transistor (BJT) with high dc current gain in 4H-SiC. BJT devices with an active area of 3/spl times/3 mm/sup 2/ showed a forward on-current of 30 A, which corresponds to a current density of 333 A/cm/sup 2/, at a forward voltage drop of 2 V. A common-emitter current gain of 40, along with a low specific on-resistance of 6.0m/spl Omega//spl middot/cm/sup 2/ was observed at room temperature. These results show significant improvement over state-of-the-art. High temperature current-voltage characteristics were also performed on the large-area bipolar junction transistor device. A collector current of 10A is observed at V/sub CE/=2 V and I/sub B/=600 mA at 225/spl deg/C. The on-resistance increases to 22.5 m/spl Omega//spl middot/cm/sup 2/ at higher temperatures, while the dc current gain decreases to 30 at 275/spl deg/C. A sharp avalanche behavior was observed at a collector voltage of 1000 V. Inductive switching measurements at room temperature with a power supply voltage of 500 V show fast switching with a turn-off time of about 60 ns and a turn-on time of 32 ns, which is a result of the low resistance in the base.
The paper presents the reliability of MOS-based 4H-SiC devices. Recent high temperature gate oxide breakdown measurements on MOS capacitors reveal that the gate oxides on an as-grown epi surface are more reliable than those grown on ion-implanted and activated surfaces. The reduction in the oxide reliability on implanted surfaces is primarily due to the deterioration of surface morphology as a result of implant damage. In addition, preliminary measurements on forward I-V characteristics and threshold voltage of power MOSFETs under a constant applied gate voltage of +20 V show the devices to be stable up to 88 hrs of operation at room temperature.
Two previously reported MOS processes, oxidation in the presence of metallic impurities and annealing in nitric oxide (NO), have both been optimized for compatibility with conventional 4H-SiC DMOSFET process technology. Metallic impurities are introduced by oxidizing in an alumina environment. This Metal Enhanced Oxidation (MEO) yields controlled oxide thickness (tOX) and robustness against high temperature processing and operation while maintaining high mobility (69 cm2/Vs) and near ideal NMOS C-V characteristics. Raising the NO anneal temperature from 1175oC to 1300oC results in a 67% increase in the mobility to 49 cm2/Vs with a slight stretch-out in the NMOS C-V. Both processes exhibit a small 30% mobility reduction in MOSFETs fabricated on NA = 1x1018 cm-3 implanted p-wells. The low field mobility in the MEO MOSFETs is observed to increase dramatically with measurement temperature to 160 cm2/Vs at 150oC.
Degradation in both current gain and specific on-resistance of fabricated 4H-SiC BJTs have been observed after a short period of operation. In this paper, 1200 V BJTs were stressed and factors that cause the degradation are proposed. The degradation may be attributed to the increase of the surface states density along the SiC/SiO 2 interface, which results in an increased surface recombination current and hence the degradation of the SiC BJT.
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