1. Unveiling microstructural damage for leakage current degradation in SiC Schottky diode after heavy ions irradiation under 200 V.
- Author
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Yan, Xiaoyu, Zhai, Pengfei, Yang, Chen, Zhao, Shiwei, Nan, Shuai, Hu, Peipei, Zhang, Teng, Chen, Qiyu, Xu, Lijun, Li, Zongzhen, and Liu, Jie
- Subjects
ELECTRON energy loss spectroscopy ,STRAY currents ,SCHOTTKY barrier diodes ,HEAVY ions ,RADIATION damage ,RAYLEIGH-Taylor instability - Abstract
Single-event burnout and single-event leakage current (SELC) in silicon carbide (SiC) power devices induced by heavy ions severely limit their space application, and the underlying mechanism is still unclear. One fundamental problem is lack of high-resolution characterization of radiation damage in the irradiated SiC power devices, which is a crucial indicator of the related mechanism. In this Letter, high-resolution transmission electron microscopy (TEM) was used to characterize the radiation damage in the 1437.6 MeV
181 Ta-irradiated SiC junction barrier Schottky diode under 200 V. The amorphous radiation damage with about 52 nm in diameter and 121 nm in length at the Schottky metal (Ti)–semiconductor (SiC) interface was observed. More importantly, in the damage site the atomic mixing of Ti, Si, and C was identified by electron energy loss spectroscopy and high-angle annular dark-field scanning TEM. It indicates that the melting of the Ti–SiC interface induced by localized Joule's heating is responsible for the amorphization and the possible formation of titanium silicide, titanium carbide, or ternary phases. The mushroom-like hillock in the Ti layer can be attributed to Rayleigh–Taylor instability, as another evidence for ever-happened localized melting near the Schottky interface. These modifications at nanoscale in turn cause localized degradation of the Schottky contact, resulting in permanent increase in leakage current. This experimental study provides very valuable clues for a thorough understanding of the SELC mechanism in SiC diodes. [ABSTRACT FROM AUTHOR]- Published
- 2024
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