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基于高能Ta离子辐照研究了SiC肖特基势垒二极管的失效模式和机理, 实验表明辐照过程中的反向偏置电压是影响SiC肖特基势垒二极管器件失效的关键因素. 当器件反向偏置在400 V时, 重离子会导致器件的单粒子烧毁, 辐照后的器件出现了因SiC材料熔融形成的“孔洞”; 当器件反向偏置在250—300 V时, 器件失效表现为关态漏电流随着离子注量增加而增加, 且器件的偏压越高, 重离子导致的漏电增加率也越高. 对于发生漏电增加的器件, 基于显微分析技术发现了分布在整个有源区内重离子导致的漏电通道. TCAD仿真结果表明, 重离子入射会导致器件内部的晶格温度上升, 且最大晶格温度随着偏置电压的增加而增加. 当偏置电压足够大时, 器件内部的局部晶格温度达到了SiC材料的熔点, 最终导致单粒子烧毁; 当偏置电压较低时, 重离子入射导致的晶格温度增加低于SiC材料的熔点, 因此不会造成烧毁. 但由于器件内部最大的晶格温度集中在肖特基结附近, 且肖特基金属的熔点要远低于SiC材料, 因此这可能导致肖特基结的局部损伤, 最终产生漏电通路.In this paper, the failure mode and mechanism of silicon carbide (SiC) Schottky barrier diode (SBD) irradiated by high-energy tantalum (Ta) ions are studied. The experimental results show that the reverse bias voltage during irradiation is the key factor causing the failure of SiC SBDs. When the reverse bias of the device is 400 V, the heavy ions will cause the single event burnout (SEB), and a “hole” formed by the melting of SiC material appears in the irradiated device. When the reverse bias is 250–300 V, the failure is manifested as the off state leakage current increases with the ion fluence. The higher the bias voltage of the device, the higher the leakage increase rate caused by heavy ions. For the devices with increased leakage, the leakage channels caused by heavy ions are found in the whole active region, based on microscopic analysis. The TCAD simulation results show that the incidence of heavy ions will lead the lattice temperature to increase in the device, and the maximum lattice temperature increases with bias voltage increasing. When the bias voltage is large enough, the local lattice temperature inside the device reaches the melting point of SiC material, resulting in SEB. When the bias voltage is relatively low, the lattice temperature is lower than the melting point of SiC material, so it will not cause burnout. However, the maximum lattice temperature in the device is concentrated near the Schottky junction, and the melting point of Schottky metal is much lower than that of SiC material. This may lead the Schottky junction to damage locally and eventually produce leakage path.
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Keywords:
- SiC power device /
- Schottky barrier diode /
- heavy ion radiation effect
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[1] Casady J B, Johnson R W 1996 Solid-State Electron. 39 1409Google Scholar
[2] Kimoto T, Cooper J A 2014 Fundamentals of Silicon Carbide Technology: Growth, Characterization, Devices and Applications (Singapore: John Wiley & Sons Press) p16
[3] 张林, 肖剑, 邱彦章, 程鸿亮 2011 物理学报 60 056106Google Scholar
Zhang L, Xiao J, Qiu Y Z, Cheng H L 2011 Acta Phys. Sin. 60 056106Google Scholar
[4] Ino K, Miura M, Nakano Y, Aketa M, Kawamoto N 2019 IEEE International Conference on Electron Devices and Solid-State Circuits (EDSSC) Xi'an, China, June 12–14 2019 p1
[5] 张鸿, 郭红霞, 潘霄宇, 雷志锋, 张凤祁, 顾朝桥, 柳奕天, 琚安安, 欧阳晓平 2021 物理学报 70 162401Google Scholar
Zhang H, Guo H X, Pan X Y, Lei Z F, Zhang F Q, Gu Z Q, Liu Y T, Ju A A, Ouyang X P 2021 Acta Phys. Sin. 70 162401Google Scholar
[6] Yu C H, Wang Y, Bao M T, Li X J, Yang J Q, Tang Z H 2021 IEEE Trans. Electron. Dev. 68 5034Google Scholar
[7] Yu C H, Wang Y, Li X J, Liu C M, Luo X, Cao F 2018 IEEE Trans. Electron. Dev. 65 5434Google Scholar
[8] McPherson J A, Kowal P J, Pandey G K, Chow T P, Ji W, Woodworth A A 2019 IEEE Trans. Nucl. Sci. 66 474Google Scholar
[9] Ball D R, Hutson J M, Javanainen A, Lauenstein J M, Galloway K F, Johnson R A, Alles M L, Sternberg A L, Sierawski B D, Witulski A F, Reed R A, Schrimpf R D 2020 IEEE Trans. Nucl. Sci. 67 22Google Scholar
[10] Akturk A, McGarrity J M, Goldsman N, Lichtenwalner D, Hull B, Grider D, Wilkins R 2018 IEEE Trans. Nucl. Sci. 65 1248Google Scholar
[11] Witulski A F, Ball D R, Galloway K F, Javanainen A, Lauenstein J M, Sternberg A L, Schrimpf R D 2018 IEEE Trans. Nucl. Sci. 65 1951Google Scholar
[12] Zhou X, Jia Y, Hu D, Wu Y 2019 IEEE Trans. Electron. Dev. 66 2551Google Scholar
[13] Soelkner G, Kaindl W, Treu M, Peters D 2007 Mater. Sci. Forum 556 851Google Scholar
[14] Martinella C, Natzke P, Alia R G, Kadi Y, Niskanen K, Rossi M, Jaatinen J, Kettunen H, Tsibizov A, Grossner U, Javanainen A 2022 Microelectron. Rel. 128 114423Google Scholar
[15] Martinella C, Ziemann T, Stark R, Tsibizov A, Voss K O, Alia R G, Kadi Y, Grossner U, Javanainen A 2020 IEEE Trans. Nucl. Sci. 67 1381Google Scholar
[16] Javanainen A, Galloway K F, Nicklaw C, Bosser A L, Ferlet-Cavrois V, Lauenstein J M, Pintacuda F, Reed R A, Schrimpf R D, Weller R A, Virtanen A 2017 IEEE Trans. Nucl. Sci. 64 415Google Scholar
[17] Mizuta E, Kuboyama S, Abe H, Iwata Y, Tamura T 2014 IEEE Trans. Nucl. Sci. 61 1924Google Scholar
[18] Javanainen A, Muinos H V, Nordlund K, Djurabekova F, Galloway K F, Turowski M, Schrimpf R D 2018 IEEE Trans. Device Mater. Reliab. 18 481Google Scholar
[19] 于庆奎, 张洪伟, 孙毅, 梅博, 魏志超, 李晓亮, 王贺, 吕贺, 李鹏伟, 曹爽, 唐民 2019 现代应用物理 10 010602Google Scholar
Yu Q K, Zhang H W, Sun Y, Mei B, Wei Z C, Li X L, Wang H, Li P W, Cao S, Tang M 2019 Modern Appl. Phys. 10 010602Google Scholar
[20] Ziegler J F, Ziegler M D, Biersack J P 2010 Nucl. Instrum. Meth. Phys. Res. B 268 1818Google Scholar
[21] Synopsys 2014 Sentaurus Device User Guide (Mountain View, CA: Synopsys Inc.) p53
[22] Shoji T, Nishida S, Hamada K, Tadano H 2014 Jap. J. Appl. Phys. 53 04EP03Google Scholar
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