Abstract

Wide bandgap (WBG) semiconductors are becoming more widely accepted for use in power electronics due to their superior electrical energy efficiencies and improved power densities. Although WBG cubic silicon carbide (3C-SiC) displays a modest bandgap compared to its commercial counterparts (4H-silicon carbide and gallium nitride), this material has excellent attributes as the WBG semiconductor of choice for low-resistance, reliable diode and MOS devices. At present the material remains firmly in the research domain due to numerous technological impediments that hamper its widespread adoption. The most obvious obstacle is defect-free 3C-SiC; presently, 3C-SiC bulk and heteroepitaxial (on-silicon) display high defect densities such as stacking faults and antiphase boundaries. Moreover, heteroepitaxy 3C-SiC-on-silicon means low temperature processing budgets are imposed upon the system (max. temperature limited to ~1400 °C) limiting selective doping realisation. This paper will give a brief overview of some of the scientific aspects associated with 3C-SiC processing technology in addition to focussing on the latest state of the art results. A particular focus will be placed upon key process steps such as Schottky and ohmic contacts, ion implantation and MOS processing including reliability. Finally, the paper will discuss some device prototypes (diodes and MOSFET) and draw conclusions around the prospects for 3C-SiC devices based upon the processing technology presented.

Highlights

  • Power electronics is a key enabling technology for energy generation, transmission, distribution and motion

  • These factors are of the utmost importance when considering that it is the automotive sector that is driving the widespread uptake of Wide bandgap (WBG) technologies

  • Schottky contact processing on 3C-SiC has mainly been conducted on heteroepitaxy utilising high work function metals such as Au or Pt. These rectifying contacts are typically characterised by high leakage currents arising from stacking faults (SFs) and antiphase boundaries (APBs) and it is clear that a step-change in material quality is needed for power device applications

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Summary

Introduction

Power electronics is a key enabling technology for energy generation, transmission, distribution and motion. 3C-SiC has a smaller energy bandgap compared to its wide bandgap counterparts such as 4H-SiC and GaN, this material displays isotropy for many of the desired power device material characteristics such as avalanche coefficients and high electron mobility [9,10] Another advantage of 3C-SiC is its relatively large thermodynamic stability meaning that bulk material can be grown at reduced thermal budgets (below 1500 ◦C). These key performance indicators for power semiconductors quantify the minimum conduction loss during DC operation (BFOM) and the minimum conduction loss at high frequencies (BHFFOM) Examination of these values suggests that lower resistance devices are possible based on 4H-SiC and GaN when compared to 3C-SiC. Fitting these impact ionisation coefficients to the electric field and substituting into the impact ionisation integral leads to closed-form solutions of the breakdown voltage and depletion layer width These material parameters allow for the initial stages of power device design. These measurements showed that antiphase boundaries (APBs) are the main defects responsible for reverse leakage current, while both APBs and stacking faults (SFs) worked as preferential current paths under forward bias of the contact

Extraction Method
Ion Implantation and Activation
Ohmic Contact
MOS Processing
PiN Diode
MOSFET
Findings
Conclusions
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