I. Introduction
Normally-off GaN-based devices have gained increasing attention in high-frequency power switching applications for the fail-safe operation and simplified gate drive topology [1]–[3]. Among several normally-OFF technologies [4]–[8], the p-GaN gate solution has played a leading role in the commercial market with a good balance among performance, reliability, and cost. Two types of gate contact between the gate metal and -GaN layer are adopted in commercial products, i.e., Ohmic-type [9] and Schottky-type [10]. In particular, the -GaN gate HEMTs with an ohmic-type gate contact have presented impressive stability and reliability [11], [12]. A Schottky gate contact to -GaN layer is the other approach for the merits of reduced gate leakage current and a larger gate swing [10]. However, the -GaN layer sandwiched between a Schottky junction and a heterojunction is electrically floating, and charges (electrons and holes) storage/emission within the floating -GaN layer would induce threshold voltage () instability under both gate stress [13], [14] and drain stress [15], [16]. Moreover, the reverse-biased Schottky junction under a positive (forward) gate bias would withstand a high electric field that causes reliability concerns. There have been extensive studies on the gate degradation of the -GaN gate HEMTs under dc static gate stress. Wu et al. [17] has reported the positive temperature-dependent gate breakdown and related it to avalanche multiplication in the space charge region near the Schottky metal/-GaN interface. Rossetto et al. [18] and Stockman et al. [19] have shown that the -GaN gate presented a time-dependent dielectric breakdown (TDDB) like degradation, following Weibull or lognormal distribution, respectively. The time-dependent gate degradation was ascribed to the formation of a percolation path in the depletion region of the -GaN layer [18]–[24].