Exploring current conduction mechanisms in 6 MeV $\text{Si}^{3+}$ ion irradiated Au/SiO2/beta-Ga2O3 metal-oxide-semiconductor devices

N. Manikanthababu, B. R. Tak, Hardhyan Sheoran, K. Prajna, B. Panigrahi, R. Singh
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引用次数: 5

Abstract

Wide bandgap and cost-effective features place Ga2O3 as a viable candidate for various power electronic devices. Au/SiO2/beta-Ga2O3 metal-oxide-semiconductor devices are tested for radiation response with 6 MeV $\text{Si}^{3+}$ ions. The leakage current density is found to increase from $8.6\times 10^{-5} \mathrm{A}/\text{cm}^{2}$ (for pristine device) to $9.8\times 10^{-4}\mathrm{A}/\text{cm}^{2}$ (at $5\times 10^{16}\ \text{ions}/\text{cm}^{2}$ fluence) at −10 V. Various current conduction mechanisms are explored under gate and substrate injection in these devices. Under gate injection, the direct tunneling dominates at low voltage regime of 0 to −3 V at all fluences due to low SiO2 thickness $(\sim 10\ \text{nm})$. The Poole-Frenkel emission is quite dominant at $5\times 10^{16}\text{ions}/\text{cm}^{2}$ attributed to the increased number of trap states in SiO2, and the estimated shallow trap depth is 0.4 (pristine) to 0.2 eV (highest fluence) from the conduction band edge. The barrier height (BH) of SiO2/beta-Ga2O3 interface estimated from the Fowler-Nordheim tunneling under substrate injection is 2.52 eV for the pristine device and the BH is found to decrease to 1.83 eV at $1\times 10^{16}\ \text{ions}/\text{cm}^{2}$ fluence.
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研究6 MeV $\text{Si}^{3+}$离子辐照Au/SiO2/beta-Ga2O3金属氧化物半导体器件的电流传导机制
宽带隙和低成本的特性使Ga2O3成为各种电力电子器件的可行候选材料。对Au/SiO2/beta-Ga2O3金属氧化物半导体器件在6 MeV {\text}{3+}$离子下的辐射响应进行了测试。发现泄漏电流密度从$8.6\乘以10^{-5}\mathrm{A}/\text{cm}^{2}$(对于原始设备)增加到$9.8\乘以10^{-4}\mathrm{A}/\text{cm}^{2}$(在$5\乘以10^{16}\ text{ions}/\text{cm}^{2}$的电压下)。研究了这些器件在栅极注入和衬底注入下的各种电流传导机制。在栅极注入下,由于低SiO2厚度$(\sim 10\ \text{nm})$,在0 ~−3 V的低电压范围内,直接隧穿在所有影响下都占主导地位。在$5\ × 10^{16}\text{ions}/\text{cm}^{2}$处,由于SiO2中陷阱态数量的增加,Poole-Frenkel发射占主导地位,估计浅陷阱深度为0.4(原始)至0.2 eV(最高通量)。在衬底注入条件下,通过fower - nordheim隧穿计算得到的SiO2/beta-Ga2O3界面势垒高度(BH)为2.52 eV,在1\ × 10^{16}\ \text{ions}/\text{cm}^{2}$的通量下,BH降至1.83 eV。
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