高电子迁移率晶体管
钝化
材料科学
物理
立体化学
晶体管
化学
图层(电子)
纳米技术
电压
量子力学
作者
Jiawei Cui,Jin Wei,Maojun Wang,Yanlin Wu,Junjie Yang,Teng Li,Jingjing Yu,Han Yang,Xuelin Yang,Jinyan Wang,Xiaosen Liu,Daisuke Ueda,Bo Shen
标识
DOI:10.1109/iedm45741.2023.10413742
摘要
This work demonstrates the E-mode active-passivation p-GaN gate HEMTs (AP-HEMTs) on sapphire substrate with blocking capabilities up to 6500 V. The AP-HEMT features an active passivation (i.e. a thinned p-GaN layer) extending from the gate edge towards near the drain contact. The 2DEG under the p-GaN gate and the active passivation is fully depleted at zero gate bias, resulting in E-mode operation with a V th = 0.8 V at I D = 10 μA/mm. With a positive V GS of 3.5 V, the AP-HEMT with L GD = 77 μm presents an R ON of 38.2 Ω-mm, and R ON,SP of 33.62 mΩ·cm 2 . In the OFF-state, the active passivation is depleted from the drain side towards the gate edge. For L GD = 77 μm, the AP-HEMT presents a high breakdown voltage of 6573 V, resulting in a FOM (BV 2 /R ON ) of 1.29 GW/cm 2 that approaches the SiC limit. In the AP-HEMT, the effect of surface charges is screened by the active passivation layer, resulting in ultralow dynamic R ON . For the AP-HEMT with L GD = 77 μm, the measured dynamic R ON /static R ON is 1.15 after a 10-ms 3000-V V DS-OFF stress (delay time = 150 μs) and 1.02 after a 3-s 4500-V V DS-OFF stress (delay time = 300 ms). The results demonstrate that the active passivation can extend the E-mode p-GaN gate HEMT technology to kV-level applications.
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