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In a ${p}$ -channel field-effect-transistor (${p}$ -FET) bridge HEMT device recently realized on a commercial ${p}$ -GaN/AlGaN/GaN-on-Si power HEMT epi-wafer, it is revealed that the device’s reverse-conduction turn-on voltage (${V}_{\text {RT}}$) can be effectively decoupled from the forward threshold voltage (${V}_{\text {TH}}$) of Schottky-type ${p}$ -GaN gate HEMTs. Unlike the conventional Schottky-type ${p}$ -GaN gate HEMTs, of which ${V}_{\text {RT}}$ is closely linked to ${V}_{\text {TH}}$ , the ${p}$ -FET-bridge HEMT enables separate designs of ${V}_{\text {RT}}$ and $V_{\text {TH}}$ so that low-loss reverse conduction and high threshold voltage can be simultaneously realized. In addition, ${V}_{\text {RT}}$ can be further reduced by engineering the AlGaN barrier layer, which will also benefit a lower channel sheet resistance without lowering ${V}_{\text {TH}}$. [ABSTRACT FROM AUTHOR]

In this work, we demonstrate a GaN-based $\textit {p-n}$ junction gate (PNJ) HEMT featuring an ${n}$ -GaN/ ${p}$ -GaN/AlGaN/GaN gate stack. Compared to the more conventional ${p}$ -GaN gate HEMT with a Schottky junction between the gate metal and ${p}$ -GaN layer, the $\textit {p-n}$ junction can withstand higher reverse bias at the same peak electric-field as the depletion region extends to both the ${n}$ -side and ${p}$ -side, while exhibiting lower leakage current. The PNJ-HEMT shows a positive threshold voltage (${V}_{\text {TH}}$) of 1.78 V, a small gate leakage $(\sim 10^{-3}$ mA/mm @ ${V}_{\text {GS}} = {10}\,\, \text {V}$). In particular, a large forward gate breakdown voltage of 19.35 V at 25 °C and 19.70 V at 200 °C was achieved with the PNJ-gate HEMT. [ABSTRACT FROM AUTHOR]

We conducted reliability characterization under reverse-bias stress (i.e., stress at OFF-state with high VDS) on the E-mode GaN metal–insulator–semiconductor field-effect-transistors (MIS-FETs) with various substrate terminations. The MIS-FETs with floating substrate (FS) show worse threshold voltage (VTH) stability than that with a grounded substrate. A non monotonic dependence of VTH shifts and OFF-state time-to-breakdown (tbd) on the positive substrate bias (Vsub) was also observed. The underlying mechanisms are the different impacts of positive Vsub on the drift of electrons and holes during the long-term stress. An important indication is that positive-biased and FS terminations should be restricted at OFF-state in order to obtain good VTH stability in applications of the GaN MIS-FET. [ABSTRACT FROM AUTHOR]

Low-loss reverse-conducting normally- OFF double-channel AlGaN/GaN power transistor with the built-in Schottky barrier diode (SBD) has been systematically studied. This device features the MOS-gate section and SBD-anode section paralleled to an interdigital layout along the gate width direction. A common access region that conducts current at both forward and reverse ON-states is employed, which is beneficial to reduce the conduction loss. With a MOS-HEMT/SBD finger width of ${4}~\mu \text{m}/2~\mu \text{m}$ and a total width ratio of 2:1, the device exhibits a threshold voltage of +0.8 V at a drain current of ${10}~\mu \text{A}$ /mm and a low forward ON-resistance of $12.1~\Omega \cdot \text {mm}$. The Schottky metal contacts 2-DEG directly, which results in a low reverse turn-on voltage of −0.6 V (at −1 mA/mm) and low reverse ON-state voltage of −1.7 V (at −50 mA/mm). A leakage suppression MOS field plate (FP) is applied to shield the Schottky contact from the strong electric field, leading to a low OFF-state leakage current of 14 nA/mm at +100-V drain bias and a high breakdown voltage (BV) of +698 V. The finger width and the number of fingers should be optimized. A narrow finger width benefits the current sharing at the access region, while the increasing number of fingers introduces more Schottky depletion regions along the gate width direction that degrade ${R}_{ \mathrm{\scriptscriptstyle ON}}$. [ABSTRACT FROM AUTHOR]

The drain induced dynamic threshold voltage (${V}_{\textrm {th}}$) shift of a ${p}$ -GaN gate HEMT with a Schottky gate contact is investigated, and the underlying mechanisms are explained with a charge storage model. When the device experiences a high drain bias ${V}_{\textrm {DSQ}}$ , the gate-to-drain capacitance (${C}_{\textrm {GD}}$) is charged to ${Q}_{\textrm {GD}}$ (${V}_{\textrm {DSQ}}$). As the drain voltage drops to ${V}_{\textrm {DSM}}$ where ${V}_{\textrm {th}}$ is measured, ${C}_{\textrm {GD}}$ is expected to be discharged to ${Q}_{\textrm {GD}}$ (${V}_{\textrm {DSM}}$). However, the metal/ ${p}$ -GaN Schottky junction could block the discharging current, resulting in storage of negative charges in the ${p}$ -GaN layer. For the device to turn on, additional gate voltage is required to counteract the stored negative charges, resulting in a positive shift of ${V}_{\textrm {th}}$. The dynamic ${V}_{\textrm {th}}$ shift is an intrinsic and predictable characteristic of the ${p}$ -GaN gate HEMT which is linearly correlated with $\Delta \!{Q}_{\textrm {GD}}={Q}_{\textrm {GD}}$ (${V}_{\textrm {DSQ}}$) $- {Q}_{\textrm {GD}}$ (${V}_{\textrm {DSM}}$). The ${V}_{\textrm {th}}$ shift is dependent on ${V}_{\textrm {DSQ}}$ as well as ${V}_{\textrm {DSM}}$ , indicating that the ${V}_{\textrm {th}}$ shift is varying along the load line during a switching operation. [ABSTRACT FROM AUTHOR]

Under reverse-bias stress (i.e., OFF-state stress with ${V} _{\text {GS}} < {V}_{\text {TH}}$) with high drain voltage, ultraviolet (UV) illumination and larger negative gate bias are found to accelerate the positive shift in threshold voltage (${V}_{\text {TH}}$) of enhancement-mode GaN MIS-FETs with fully recessed gate. These results suggest a hole-induced degradation mechanism. In the absence of UV illumination, holes could be generated by impact ionization in the high electric-field region, which is initiated by electrons injected from the source through the buffer layer. With a larger negative gate bias, more holes will flow to the gate side and pass through the silicon nitride (SiNx) gate dielectric, as SiNx does not present any energy barrier to holes. The enhanced hole transport through the dielectric under large negative gate bias could accelerate new defects generation and therefore result in the larger positive threshold voltage shifts. [ABSTRACT FROM AUTHOR]

In this letter, we investigated the threshold voltage V\text {TH} stability under reverse-bias step-stress in the E-mode LPCVD-SiNx/PECVD-SiNx/GaN MIS-FET. Under the OFF-state reverse-bias stress with the same net gate-to-drain voltage ( V\text {GD} ), the V\text {TH} shift shows an obvious dependence on the negative gate bias. With a V\text {GS} of 0 V, the V\text {TH} shift is small and recoverable, while the V\text {TH} shifts are substantially larger with more negative gate bias ( V\text {GS}=-20 V). This larger V\text {TH} shifts caused by the negative V\text {GS} can be explained with a hole-induced degradation model. An important indication revealed by this model is that negative gate bias should be well confined in high-power switching applications of GaN E-mode MIS-FET for a stable V\text {TH} . [ABSTRACT FROM PUBLISHER]

GaN power switching transistors featuring MIS- and MOS-gate structures are highly preferred over the Schottky-gate counterpart, because of suppressed gate leakage, enlarged gate swing, and more scalable threshold voltage. Nevertheless, MIS-/MOS-gate GaN devices are confronted with stability and reliability challenges, which arise from interface traps at the critical dielectric/III-nitride interface, as well as bulk traps inside the gate dielectric including border traps near the critical interface. In this work, we present several key techniques toward reliable MIS-/MOS-gate GaN power devices, including advanced interface engineering technology, gate structure optimizations for high-performance/stability normally-off GaN power transistors, and long-lifetime gate dielectric technology. Schematic cross sections of GaN-based MIS-HEMT and MOS-channel-HEMT. [ABSTRACT FROM AUTHOR]