10 kV E-mode GaN HEMT: Physics for breakdown voltage upscaling
Abstract
High-voltage GaN high electron mobility transistors (HEMTs) have recently reached the 10 kV milestone; however, prior reports relied on unconventional epitaxial structures—such as multi-channel, Si delta-doping, or unintentional p-GaN doping—which pose challenges in the realization of enhancement-mode (E-mode) gate control. Here, we demonstrate a 10 kV E-mode GaN HEMT with a standard highly doped p-GaN gate. This p-GaN layer also forms a reduced-surface-field (RESURF) structure. By analyzing devices with varying RESURF thickness (tR), we identify the key physical mechanism that enables the breakdown voltage (BV) upscaling with device length. We find the BV upscaling is only viable when tR is below 21 nm and reaches peak effectiveness at a tR of 17 nm—deviating from predictions based on ideal polarization superjunction theory. This suggests the presence of donor trap states that balance the acceptors in p-GaN. Additionally, the low Mg doping near the p-GaN/AlGaN interface, naturally formed in epitaxial growth, relaxes the precision required for tR control to maintain charge balance. Under the optimal tR, we demonstrate a 10 kV GaN E-mode HEMT with a specific on-resistance (RON,SP) of 69 mΩ cm2, which is lower than the RON,SP of 10 kV SiC MOSFETs. We also test a 5 kV device under prolonged high-temperature reverse bias stress at 3 kV and 150 °C. The device shows minimal parametric shifts, manifesting electrical and thermal reliability of the underlying charge modulation. The findings offer valuable guidance for the design of multi-kilovolt GaN power HEMTs using industry-standard wafers.
Article Details
Journal Info
Applied Physics Letters
American Institute of Physics
Authors (14)
Yijin Guo
Center for Power Electronics Systems, Virginia Polytechnic Institute and State University 1 , Blacksburg, Virginia 24061,
Yuan Qin
Matthew Porter
Zineng Yang
Ming Xiao
Yifan Wang
Daniel Popa
Cambridge GaN Devices Ltd. 4 , CB4 0DS Cambridge,
Loizos Efthymiou
Cambridge GaN Devices Ltd. 4 , CB4 0DS Cambridge,
Chu Cheng
Enkris Semiconductor Inc. 5 , Suzhou 215123,
Kai Cheng
State Key Laboratory of Magnetic Resonance Spectroscopy and Imaging, National Center for Magnetic Resonance in Wuhan, Wuhan National Laboratory for Optoelectronics, Wuhan Institute of Physics and Mathematics
Ivan Kravchenko
Center for Nanophase Materials Sciences, Oak Ridge National Laboratory 6 , Oak Ridge, Tennessee 37830,
Linbo Shao
Florin Udrea
Cambridge GaN Devices Ltd. 4 , CB4 0DS Cambridge,
Yuhao Zhang