Papers by Author: Kazuo Arai

Abstract: 3 kV normally-off SiC-buried gate static induction transistors (SiC-BGSITs) were fabricated by using an innovative fabrication process that was used by us previously to fabricate 0.7–1.2 kV SiC-BGSITs. The fabricated device shows the lowest specific on-resistance of 9.16 mΩ·cm², compared to all other devices of the same class. The threshold voltage of this device was 1.4 V at room temperature and was maintained at values more than 1 V with normally-off characteristics at 200 °C. The device can block drain voltage of 3 kV with a leakage current density of 6.9 mA/cm².

Abstract: We investigated the short-circuit capabilities of 1.2 kV normally-off SiC buried gate static induction transistors (SiC-BGSITs). The maximum short-circuit energy was found to be 35.6 J/cm2, which is twice that of normally-on SiC-BGSITs and 3.3–5.6 times higher than that of the Si-IGBTs. The maximum short-circuit time was 590 μs. It is concluded that these high short-circuit capabilities result from saturation characteristics of the normally-off SiC-BGSITs.

Abstract: In this work, we succeeded in developing high performance normally-off SiC buried gate static induction transistors (SiC-BGSITs). To achieve the normally-off characteristics, design parameters around the channel region were optimized and process conditions were improved to realize these parameters. The off-state characteristic of the SiC-BGSIT showed an avalanche breakdown voltage of VBR=980 V at a gate voltage of VG=0 V. Furthermore, the leakage current at VD=950 V is lower than 0.5 μA. These results indicate that the BGSIT has a good normally-off characteristic. At VG=2.5 V, an on-resistance of 28.0 mΩ corresponding to the specific on-resistance of 1.89 mΩ•cm2 was obtained and the current rating was calculated as 33 A at a power density of 200 W/cm2 in the on-state characteristic.

Abstract: In this study, we suggest the effective enlargement method of (0001) 4H-SiC bulk crystals grown by the sublimation method using long length growth technique (LLG). This method could achieve low thermal strain and rapid enlargement growth comparing with conventional c-axis growth technique. We also demonstrated high quality enlargement growth from 2inch to  4inch of (0001) 4H-SiC by LLG.

Abstract: The authors fabricated pn diodes with Al+ implantation in p-type epitaxial layers, and investigated the influence of the implantation dose on reverse leakage currents. Only in the highest dose with the Al concentration of 2x1020cm-3, more than 90% of the devices showed high leakage currents above 10-4A at the maximum electric field of 3MV/cm. In such devices, almost all of the emissive spots corresponded to threading screw dislocations (TSDs) by the analysis of emission microscopy and X-ray topography. These TSDs were defined as killer defects with the estimated density of 500cm-2 in the case of the highest dose. The emissions were supposed to be due to microplasmas, since the spectra of the emissions were different from those of heat radiation. Condensation of Al atoms, nitrogen atoms and DI defects were excluded as the origin of the emissions by secondary ion mass spectrometry and low temperature photoluminescence analyses.

Abstract: It is known that a Schottky barrier height (b) of metal/C-face 4H-SiC Schottky barrier diode (SBD) differ from b of metal/Si-face 4H-SiC SBD. Furthermore, b of metal/4H-SiC SBD varies with annealing temperature. We fabricate 0.231mm2 SBD with Ti/SiC interface using Si-face and C-face 4H-SiC. These SBDs are annealed at several temperatures after a formation of the Ti/SiC interface. As a result, b of Ti/C-face 4H-SiC interface annealed at 400 oC is nearly equal to b of Ti/Si-face 4H-SiC interface annealed at 500 oC and the n-values of these SBDs are nearly equal to the ideal value (unity). Using that annealing condition, we fabricated 25mm2 junction barrier Schottky (JBS) diodes with Ti/SiC interface on Si-face and C-face 4H-SiC epitaxial substrate. b of Si-face and C-face JBS diodes are 1.26eV and 1.24eV, respectively. The leakage currents for both Si-face and C-face JBS diodes are less than 1mA/cm2. The current of 100A is obtained at the forward bias voltage of 1.95V and 2.16V for the Si-face JBS and the C-face JBS.

Abstract: The effect of ammonia (NH3) post-oxidation annealing (POA) technique on the reliability of thermal oxides grown on a n-type 4H-SiC (0001) face by dry oxidation has been investigated. Comparing other POA techniques using hydrogen and nitrous oxide gases, it was indicated that the NH3 POA after dry oxidation remarkably improves the insulating properties of thermal oxides. The mode value of field-to-breakdown for thermal oxides prepared by NH3 POA was 12.1 MV/cm. The charge-to-breakdown (QBD) in the NH3 POA sample was the highest in all samples, and the QBD value at 63% cumulative failure rate was 19.1 C/cm2. In addition, the NH3 POA maintained excellent electron trapping characteristics of thermal oxides against the electron injection.

Abstract: This paper discusses the issues regarding reliability of large-area (up to 25mm2) gate oxide on the C-face of 4H-SiC. We have shown that the TDDB characteristics of large-area gate oxide improved by separating gate oxidation processes into oxide growth by dry-oxidation and successive interface control by anneal in N2O ambient or that by wet-oxidation followed by anneal in H2 ambient. In particular, dry-oxidation followed by anneal in N2O ambient for interface treatment (dry+N2O process) is effective for the suppression of the random failure in TDDB characteristics. The estimated lifetime of gate oxide of less than 9mm2 by the dry+N2O process is six-digits larger than 30 years. In the case of the TDDB characteristics of 25mm2 gate oxide grown by the dry+N2O process, the initial and random failure in TDDB characteristics is dominant. However, even in this case, we have confirmed that the evaluated lifetime of 25mm2 gate oxide is more than 30 years. In order to clarify the mechanism of the degradation of the TDDB characteristics of large-area gate oxide, we examined the effect of the surface defect on the TDDB characteristics by observing the surface of each broken MOS capacitor after the TDDB test. We have found following results. (1) The initial failures in TDDB characteristics are mainly due to surface defects such as “down fall”, “comet”, and “triangular defect”. (2) The footprints of random failure do not correspond to the positions of smaller surface defects such as “bump”. Finally, we have found that the quality of the epitaxial layer affects random failure rate in the TDDB characteristics of large area gate oxide; the random failure in the TDDB characteristics of 25mm2 gate oxide on epitaxial layer grown by a certain epitaxial vendor is almost suppressed. However, the cause of the difference in TDDB characteristics is not identified.

Abstract: The influences of processing and material defects on the electrical characteristics of large-capacity (approximately 100A) SiC-SBDs and SiC-MOSFETs have been investigated. In the case of processing defects, controlled activation annealing is the most important factor. On the other hand for material defects, the number of epitaxial defects must be decreased to zero for both SBDs and MOSFETs. The dislocation defects in SiC wafers are dangerous for the breakdown voltage of MOSFETs. However, they are not killer defects. If the epitaxial defect density is sufficiently low and the dislocation density is in the order of 10000cm-2, the long- term reliability of the gate oxide at the electric field of 3MV/cm can be guaranteed.

Abstract: In this study, we investigated the cluster effect on the occurrence of giant step bunching. We generated carbon clusters on 4H-SiC (0001) surfaces by thermal decomposition of SiC in an Ar atmosphere and controlled the surface concentrations of the clusters by adding H2 gas. We found the boundaries between surfaces with and without giant steps to show Arrhenius-type behavior. This behavior agreed with our predictions deduced from a chemical reaction model that takes the cluster effect into account, suggesting that giant step bunching is attributable to the formation of clusters on SiC.