Silicon-based insulated gate bipolar transistors (IGBTs) are often regarded as the "CPU" of electrical systems due to their ease of control, high voltage, and high current capabilities. The IGBT is a unidirectional device and needs to be co-packaged with an anti-parallel diode for current freewheeling in inductive loads. They are widely used in power conversion and motor drive hard-switching applications because of their high current density and cost-effectiveness. Reverse conducting IGBTs (RC-IGBTs) incorporate both the IGBT and antiparallel diode into a single chip, offering low cost, compact size, high reliability, and low thermal resistance. However, the application of RC-IGBTs in hard-switching is limited due to the conflicting requirements in carrier distribution between the IGBT and diode modes of operations. To improve the reverse recovery characteristics of RC-IGBTs in the diode mode, it is crucial to lower the reverse recovery loss (E
rec) to reduce switching power loss, decrease the reverse recovery time (T
rr) to support higher switching frequencies, improve the softness factor (S) for effective electromagnetic interference control, and reduce the peak reverse recovery current (I
rrm) to enhance device reliability. This thesis presents the design and characterization of a novel RC-IGBT with superior reverse recovery characteristics for hard-switching applications such as motor drive inverters.
First, the novel RC-IGBT incorporates critical structures such as a punch-through (PT) NPN and a JFET for electron extraction (EE). These structures were designed and experimentally validated by fabricating a discrete PT-NPN diode. Compared with a conventional Self-adjusting P Emitter Efficiency Diode (SPEED), the proposed PT-NPN diode provides a much larger S (+23%), a shorter T
rr (-5%), and a much reduced reverse recovery charge Q
rr (-20%) at a nominal current. Second, the analysis and characterization of the PT-NPN diode are further performed. Numerical analysis shows that the PT voltage V
PT and the P
+ width ratio are critical parameters to control the hole injection efficiency of the PT-NPN diode. Experimental results show that the leakage current of the PT-NPN diode at 400 K can be kept at a level similar to that of the conventional SPEED with a well-designed V
PT. Compared with SPEED, the PT-NPN diode achieves a reduced I
rrm (-21%) and minimized E
rec (-18%) at a nominal current. It can realize a significantly reduced I
rrm (-42%) even at a small current and a bus voltage of 800 V. Moreover, the better reverse recovery performances of the PT-NPN diode can be maintained at 450 K. Third, the electron extraction mechanism of the PT-NPN diode is fully investigated. Similar to the N-type Schottky barrier, the PT-NPN region in the PT-NPN diode features a unipolar structure for electron unidirectional conduction. Experimental results show that S of the PT-NPN diode is increased by 20% compared with that of a N-Schottky implemented PT-NPN (N-Schottky PT-NPN) diode. In addition, the PT-NPN diode attains a stable BV of 1268 V with a low leakage current; however, the leakage current of the N-Schottky PT-NPN diode is increased by 10 times when the barrier height is varied by 0.3 eV. Finally, the fabrication compatibility of the PT-NPN and JFET structures with conventional RC-IGBT is evaluated, and a new EE RC-IGBT is proposed to enhance the reverse recovery characteristics in the diode mode for hard-switching applications. During the IGBT mode of operation, the EE RC-IGBT demonstrates similar threshold voltage and short circuit capability compared to those of the conventional Floating P-body (FP) RC-IGBT. For reverse conduction in the diode mode, the hole carriers of the EE RC-IGBT are reduced by 66% compared to that of the FP RC-IGBT due to the electron extraction effect. As a result, compared to the fabricated conventional device, the proposed device exhibits a reduction of 20% in I
rrm and 16% in E
rec at a small current. Furthermore, the proposed device shows a 19% increase in S, a 12% reduction in I
rrm, a 14% decrease in Q
rr, and a 10% reduction in E
rec at a nominal current. Experimental results also indicate that the electron extraction does not increase V
F of the proposed device, and the FP and EE RC-IGBTs in the diode mode have the same avalanche capability of absorbing an avalanche energy of 3.37 mJ.
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