20.3 A GaN Gate Driver with On-chip Adaptive On-time Controller and Negative Current Slope Detector

Monolithic gallium nitride (GaN) solutions are widely used in high power density applications, due to low on-resistance (\mathrm{R}_{\text{ON}}) and low parasitic capacitance [1-3]. However, some process defects, such as current collapse, kink effects, and self-heating (top left of Fig. 20.3.1), wil...

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Published in2023 IEEE International Solid-State Circuits Conference (ISSCC) pp. 306 - 308
Main Authors Lin, Shu-Yung, Lin, Ssu-Yu, Hung, Sheng-Hsi, Wang, Tz-Wun, Li, Ching-Ho, Go, Chang-Lin, Huang, Shao-Chang, Chen, Ke-Horng, Zheng, Kuo-Lin, Lin, Ying-Hsi, Lin, Shian-Ru, Tsai, Tsung-Yen
Format Conference Proceeding
LanguageEnglish
Published IEEE 19.02.2023
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Summary:Monolithic gallium nitride (GaN) solutions are widely used in high power density applications, due to low on-resistance (\mathrm{R}_{\text{ON}}) and low parasitic capacitance [1-3]. However, some process defects, such as current collapse, kink effects, and self-heating (top left of Fig. 20.3.1), will degrade the \mathrm{I}_{\text{DS}}-\mathrm{V}_{\text{DS}} curve of high voltage GaN devices, which can lead to efficiency degradation and power device damage. Current collapse will increase \mathrm{R}_{\text{ON}} , which will cause the GaN to heat up causing self-heating, and the \mathrm{I}_{\mathrm{D}} current drops significantly when GaN enters the saturation region. Furthermore, the kink effect induced by hot electrons trapped by donor-like traps through the GaN buffer will induce a negative slope in the triode region, which may lead to blurred transitions from the triode region to the saturation region. Thus, if the detection of saturation is inaccurate, the sudden change from the kink effect to self-heating will limit the current driving capability. Consequently, in flyback converters, part of the inductor current will leak to the secondary side when the primary side GaN is still turned on, resulting in serious shoot-through effects.
ISSN:2376-8606
DOI:10.1109/ISSCC42615.2023.10067355