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III-nitride heterostructure-based metal–insulator–semiconductor high-electron-mobility transistors (MIS-HEMTs), compared with Schottky and p-GaN gate HEMTs, have demonstrated significant potential in the next-generation high-power electronic devices due to their exceptional gate reliability. This study presents a comprehensive investigation of threshold voltage (VTH) instability in III-nitride heterostructure-based MIS-HEMTs, with a specific emphasis on the interfaces of the multi-heterostructures. Two widely studied amorphous materials, namely, Al2O3 and SiNx, have been extensively examined as primary gate insulators in GaN-based MIS-HEMTs. To efficiently remove native oxides from the (Al)GaN surface, a novel in situ high-temperature remote plasma pretreatment (RPP) technique has been developed. This technique involves sequential application of NH3/N2 plasmas on the (Al)GaN surface before depositing the gate insulators using plasma-enhanced atomic layer deposition. The remarkable RPP process has proven to be a highly effective method for revealing atomic steps on the GaN surface, irrespective of whether the surface has undergone oxidation or etching processes. To further enhance the interface quality and potentially reduce bulk traps in the gate insulator, optimization of deposition temperature and post-deposition annealing conditions have been explored. Additionally, an electron-blocking layer, such as SiON, is incorporated into the MIS-HEMTs to prevent electron injection into bulk traps within the insulator. Novel characterization techniques including constant-capacitance and isothermal-mode deep-level transient spectroscopy have also been developed to explore the failure mechanisms in MIS-HEMTs. These techniques allow for the differentiation between bulk traps in the GaN epitaxy and those present within the gate insulators. This in-depth physical understanding provides valuable insights into the sources of failure in GaN-based MIS-HEMTs. [ABSTRACT FROM AUTHOR]

In this work, AlN polarization-enhancement interlayer (AlN-PEL) is adopted to enhance two-dimensional hole gas (2DHG) density in a p-GaN/AlN-PEL(∼2 nm)/AlGaN(<6 nm)/GaN heterostructure, aiming at monolithic integration of p/n-channel field effect transistors (p-FETs) on GaN-on-Si substrate. Owing to the strong built-in polarization of the AlN-PEL, high density 2DHG over 2.3 × 1013 cm−2 with good immunity to thermal freeze out effect is realized. Assisted by a two-step gate trench etching process, enhancement-mode (E-mode) buried-channel GaN p-FETs with temperature independent ON-resistance RON, and ON/OFF current ratio ION/IOFF (>108), have been fabricated. The fabricated p-FETs also deliver thermally stable subthreshold swing as well as threshold voltage Vth, and smaller Vth shift than that of p-FETs without the AlN-PEL, which is primarily due to enhanced 2DHG confinement by the AlN-PEL. The proposed structure is an attractive platform for monolithic integration of GaN-based logic and power devices for cryogenic applications as low as 10 K. [ABSTRACT FROM AUTHOR]

A 650-V/84-mΩ normally-off GaN/SiC cascode device is demonstrated with systematic static and dynamic characterizations. The cascode device features a low-voltage enhancement-mode (E-mode) gallium nitride (GaN) high electron mobility transistor (HEMT) to enable normally-off gate control, and a 650-V normally-on silicon carbide (SiC) JFET provides the high-voltage blocking capability. The GaN/SiC cascode device exhibits many application-desired behaviors, including reverse conduction capability, avalanche breakdown capability, thermally stable threshold voltage, low input/output capacitances, no dynamic RON degradation, and negligible dynamic VTH shift. In addition, a customized double-pulse test board is built to evaluate the switching performance of this cascode device and other 650-V SiC-based power devices. This cascode device adopting low-voltage GaN HEMT has low QG×RON and exhibits excellent switching performance. The switching losses (EON and EOFF) are much smaller than that of the 650-V Si/SiC cascode device and comparable to that of the state-of-the-art 650-V SiC MOSFETs. [ABSTRACT FROM AUTHOR]

The high-speed superiority of GaN power devices with silicon-based peripheral circuits is not yet fully leveraged, mainly due to the parasitic inductance of interconnections. In this article, we demonstrate a GaN-based gate driver with an overcurrent (OC) protection circuit and an undervoltage lockout (UVLO) circuit on a p-GaN gate power HEMT platform. The gate driver features a rail-to-rail output voltage, suppressed gate ringing, and tunable driving speed, all of which are highly desired in high-efficiency and high-speed GaN power systems. To offer timely but reliable protections, the OC protection and UVLO circuit are designed with reference to the switching speed and the threshold voltage of GaN power devices. The OC protection is implemented with a separated sensing branch and blanking time controller, and the response time to an OC event is reduced to 10 ns after the blanking time. The UVLO circuit has a fixed hysteresis of 0.5 V, and its threshold voltage is especially tailored for the GaN integrated circuits. [ABSTRACT FROM AUTHOR]

The short circuit (SC) behavior of a newly developed GaN-HEMT/SiC-JFET cascode device is investigated in this work. The reverse leakage current through the drain-side PN junction (IR) of the SiC JFET under SC conditions is measured simultaneously during the SC event. IR of the SiC JFET increases to 6.4 A at the end of a 5-μs nondestructive SC pulse. The increase of IR during the SC pulse induces a turning point in the SC current waveform and a dramatic negative threshold voltage shift (>30 V) in the SiC JEFT, resulting in high transient drain-to-source voltage in the GaN HEMT. The underlying mechanism is associated with the increase of local potential in the P-type layer of the SiC JFET with inevitable spread resistance (RSPD). It is suggested that reducing RSPD can improve SC capability and high IR should be considered in SC failure mechanism analysis and the design of external gate resistance of the SiC JFET. [ABSTRACT FROM AUTHOR]

GaN ${p}$ -channel field-effect transistors (${p}$ -FETs) are essential components for implementing the energy-efficient complementary logic circuitry for monolithic GaN power integration. This letter reports the threshold voltage (${V}_{\mathrm {TH}}$) instability of ${p}$ -channel GaN MOSFETs with Al2O3 as the gate dielectric. When the gate-to-source bias sweeps toward the negative direction, the ${V}_{\mathrm {TH}}$ exhibits a shift toward more negative values. The impacts of such ${V}_{\mathrm {TH}}$ instability on GaN complementary logic circuits are characterized using logic inverters and ring oscillators. It is shown that impacts on circuit functions are limited with an operating voltage swing below 5 V. However, the propagation delay could be gradually prolonged, as a result of the drifting ${V}_{\mathrm {TH}}$. [ABSTRACT FROM AUTHOR]

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]

The threshold voltage (VTH) of an enhancement-mode Schottky-type p-GaN gate high-electron-mobility transistor (HEMT) is found to have a special dependence on the drain bias. The device commonly requires higher gate voltage to switch on the transistor from a high-drain-voltage off-state than what is expected from the static device characteristics. The reason behind the dynamic VTH has been proved to be the floating p-GaN layer, where charges could be stored and further influence VTH under different drain bias. In this article, a SPICE-compatible equivalent circuit model is presented according to the structure of Schottky-type p-GaN gate HEMTs. It features a floating node to imitate the charge storage process within the gate stack. Compared to conventional models, the proposed model could accurately predict the dynamic VTH characteristics and switching behaviors of power electronics circuits, where Schottky-type p-GaN gate HEMTs are deployed as power transistors. The phenomena related to the dynamic VTH, including the disappearance of Miller plateau, the overestimated false-turn-on problem, and the higher reverse conduction loss are evaluated with a half-bridge circuit and the merits of the proposed model are verified. [ABSTRACT FROM AUTHOR]

In this work, the impact ionization-induced OFF-state breakdown is revealed and systematically investigated in 100 V Schottky-type p-GaN gate high-electron-mobility transistors. Impact ionization is found to occur in the peak electric-field region at the source-terminated field-plate edge and is initiated by electrons injected from the source-side two-dimensional electron gas channel through the buffer layer. Hot electrons generated from impact ionization, when being captured by surface traps, could lead to redistribution and peak value reduction of electric-field. Consequently, the sudden rise in the OFF-state leakage current by impact ionization could be self-clamped temporally to avoid catastrophic rupture of the device. The impact ionization is further verified by the increase in dynamic OFF-state leakage current and a negative shift in threshold voltage, both of which result from positively charged holes (generated from impact ionization) drifting toward the gated channel. [ABSTRACT FROM AUTHOR]

The dynamics of the intrinsic threshold voltage (VTH) shift in 650-V Schottky-type p-GaN gate HEMT under high-frequency switching is investigated by a bootstrap voltage clamping circuit in which the GaN HEMT serves as the key bootstrapping device. This new testing setup covers a wide range of OFF-state drain bias (VDSQ) up to 400V, a short OFF-to-ON (or stress-to-sense) delay (Tdelay) of 60ns, and a high switching frequency (ƒsw) up to 2MHz. The dynamic VTH’s dependences on VDSQ and ƒsw are characterized by this testing setup. A higher VDSQ (up to 400V) results in a larger dynamic VTH shift (Δ VTH). The Δ VTH exhibits a gradually increasing trend under the continuous high-frequency switching mode. In addition, after continuous switching operation for 200 μs, the maximum Δ VTH shows no ƒsw dependence with a wide range of frequency from 50kHz to 2MHz. [ABSTRACT FROM AUTHOR]

GaN power transistors are attracting increasing attention for next-generation power switching applications. However, GaN power transistors should not be regarded as a direct replacement for silicon power metal–oxide–semiconductor field-effect transistors, since the unique properties of GaN power transistors require special treatment. In this work we review a unique and critical property of GaN power transistors, the dynamic threshold voltage (Vth). GaN power transistors feature a p-GaN gate structure, while the gate metal contacts the p-GaN layer through a Schottky junction. This unique p-GaN gate structure is distinctively different from the silicon metal–oxide–semiconductor gate structure in that the p-GaN layer is actually a floating region without direct electrical contact to the external electrodes of the device. The floating p-GaN layer enables a charge storage process during the switching operation of a p-GaN gate high-electron-mobility transistor. Through carefully designed experiments, the strong correlation between charge storage and the dynamic Vth shift has been revealed; this also serves as an approach to accurately predict the dynamic Vth during switching operation. The influence of the dynamic Vth on power switching applications is discussed. For example, with a positive dynamic Vth shift, the reverse conduction voltage of a GaN power transistor is significantly increased, adding to the power loss. This positive Vth shift also demands a sufficiently high gate drive voltage to ensure that the GaN power transistor can be fully turned on, which reduces the safety margin for the gate reliability of the device. To design a GaN based power switching circuit, accurate simulation of the device/circuit characteristics is necessary. Circuit simulations that do not consider the dynamic Vth lead to a large deviation from the measurement circuit characteristics. We demonstrate that by incorporating the dynamic Vth into the circuit model this deviation can be effectively eliminated. [ABSTRACT FROM AUTHOR]

A gallium nitride (GaN) ring oscillator based on high-performance one-chip complementary logic (CL) inverters is demonstrated on a conventional ${p}$ -GaN gate power HEMT (high-electron-mobility transistor) platform. It manifests the feasibility of the multiple-stage monolithic integration of GaN CL gates, the most energy-efficient digital circuit configuration, and consequently the potential of deploying CL circuits in the all-GaN power integration as peripheral circuits with higher energy efficiency. Thanks to the successful monolithic integration of enhancement-mode ${p}$ -channel and ${n}$ -channel field-effect transistors, the integrated CL inverters in this work present remarkable performances, including stringent rail-to-rail operations, substantially suppressed static power dissipation at both logic ‘low’ and ‘high’ states, suitable transition threshold voltages of ~2.0 V (40% of the common 5-V supply) and wide noise margins above 1.8 V (36% of 5 V). [ABSTRACT FROM AUTHOR]

By deploying a surface reinforcement layer (SRL) at the interface between Schottky metal and ${p}$ -GaN in the gate stack, a ${p}$ -GaN gate high-electron-mobility transistor (HEMT) with enhanced gate reliability is demonstrated. Prior to the gate metal deposition, the SRL is formed by an oxygen-plasma treatment and a subsequent high-temperature annealing process (at 800 °C) that enables surface reconstruction. Such a process converts several nanometers of ${p}$ -GaN near the surface into a crystalline GaON layer, which exhibits stronger immunity to hot electron bombardment. With nearly identical threshold voltage and ON -resistance, the ${p}$ -GaN gate HEMT with SRL yields two orders of magnitude reduction in gate leakage current at ON -state and an increase from 10.5 V to 12.7 V in forward gate breakdown voltage. Time-dependent gate breakdown measurement reveals an increase from 5.9 V to 7.8 V in the maximum ON -state gate drive voltage for a 10-year lifetime with a 1 % gate failure rate, which effectively expands the operating voltage margin of the ${p}$ -GaN gate power HEMT. [ABSTRACT FROM AUTHOR]

Systematic characterizations of a cascode device with a low-voltage enhance-mode (E-mode) p-GaN gate high-electron mobility transistor as the control device and a high-voltage (HV) depletion-mode (D-mode) silicon carbide junction field effect transistor (JFET) as the voltage blocking device are presented in this article. The demonstrated device with a breakdown voltage rating of 1200 V and a static on-resistance (RON) of 100 mΩ features small device capacitances with fast switching speed, avalanche breakdown capability, thermally stable threshold voltage (VTH), and no dynamic RON degradation. To identify its safe operation in the off-state with a high drain bias, the off-state middle point voltage (VM) between the E-mode device drain and D-mode device source is investigated. A relatively low off-state VM is achieved under both static and dynamic modes. In addition to the device-level characterization, a custom-designed double-pulse test circuit is built to evaluate the transient switching performance of the cascode device. Optimal gate drive conditions are proposed to 1) overcome the drain bias induced positive dynamic VTH shift; and 2) suppress the increased dynamic off-state leakage current (IOFF) induced by on-state hole injection. Under 800 V/16 A testing conditions, high switching speed with the drain voltage peak slew rates of 72 V/ns during turn-on and 121 V/ns during turn-off is achieved. [ABSTRACT FROM AUTHOR]

A 1200-V/100-mΩ silicon carbide (SiC) junction field-effect-transistor (JFET)/ gallium nitride (GaN) high-electron-mobility-transistor (HEMT) hybrid power switch is demonstrated, which features a flip-chip copackaged cascode configuration incorporating a vertical SiC JFET and a lateral GaN-HEMT. The high-voltage SiC-JFET provides the high-voltage blocking capability while the low-voltage GaN-HEMT enables the normally-off gate control with superior switching characteristics. Compared to conventional SiC-JFET/Si-mosfet cascode devices, the SiC-JFET/GaN-HEMT cascode device exhibits fast switching speed, which has been validated by systematic characterizations including static/dynamic device-level measurements and board-level hard-switching tests. Meanwhile, the device is free from several notorious issues of high-voltage GaN power transistors such as dynamic on-state resistance degradation and threshold voltage shift. Such a wide-bandgap semiconductor-based hybrid switch is suitable to be deployed in high-power and high-efficiency power conversion systems. [ABSTRACT FROM AUTHOR]

In this work, the deep-level transient spectroscopy (DLTS) is conducted to investigate the gate stack of the p-GaN gate HEMT with Schottky gate contact. A metal/p-GaN/AlGaN/GaN heterojunction capacitor is prepared for the study. The DLTS characterization captures the transient capacitance change in the stack, from which the capacitance of the metal/p-GaN Schottky junction can be extracted. By proper selection of the rate window, the impacts of the hole insufficiency effect are avoided during trap states evaluation. Thus, the information of deep energy levels in the p-GaN layer is revealed, which consists of an electron trap state with activation energy of 0.85 eV and a hole trap state with activation energy of 0.49 eV. The identification of these trap states in the p-GaN layer provides a physical foundation for understanding the threshold voltage instability in Schottky-type p-GaN gate power HEMTs. [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]

A 700-V normally-off ${p}$ -GaN gate power transistor with distributed built-in Schottky barrier diode (SBD) is demonstrated in this work. The transistor cell and diode cell are alternately arrayed along the device width and are locally isolated using ion implantations. The built-in SBD provides a low reverse turn-on voltage which is independent of the threshold voltage and gate bias of the transistor. Compared to the two-device scheme consisting of an anti-parallel ${p}$ -GaN gate HEMT/SBD pair, the proposed transistor exploits the common access region in both forward conduction and reverse conduction, thus a significant reduction in chip area is obtained. [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]

Enhancement-mode (E-mode) buried p-channel GaN metal-oxide-semiconductor field-effect-transistors (p-GaN-MOSFET’s) with threshold voltage (VTH) of −1.7 V, maximum ON-state current (ION) of 6.1 mA/mm and ION/IOFF ratio of 107 are demonstrated on a standard p-GaN/AlGaN/GaN-on-Si power HEMT substrate. An oxygen plasma treatment (OPT) was deployed to the gated p-GaN region where a relatively thick (i.e. 31 nm) GaN is retained without aggressive gate recess. The OPT converts the top portion of the GaN layer to be free of holes so that only the bottom portion remains p-type while being spatially separated from the etched GaN surface and gate-oxide/GaN interface. As a result, E-mode operation is enabled while a high-quality p-channel is retained. Multi-energy fluorine ion implantation was implemented for planar isolation of GaNp-channel FETs with mesa edges and sidewalls eliminated. Consequently, high ION/IOFF ratio is obtained. [ABSTRACT FROM AUTHOR]

In this paper, we carried out a systematic investigation on gate degradation and the physical mechanism of the Schottky-type ${p}$ -GaN gate HEMTs under positive gate voltage stress. The frequency- and temperature-dependent measurements have been conducted. It is found that the time-dependent gate degradation exhibits weak relevance with frequencies ranging from 10 to 100 kHz under dynamic gate stress and is similar to that in static gate stress. Both the gate breakdown voltage (BV) and mean-time-to-failure (MTTF) show positive temperature dependence. Moreover, the current–voltage (I–V) characteristics and threshold voltage (${V}_{\text {TH}}$) instability of ${p}$ -GaN devices before/after gate degradation are compared and analyzed. The degraded Schottky junction exhibits an ohmic-like gate behavior. It is revealed that under a large gate bias stress, high-energy electrons accelerated in the depletion region of the ${p}$ -GaN layer would promote the formation of defect levels near the metal/ ${p}$ -GaN interface, leading to the initial ${p}$ -GaN layer degradation. The subsequent high gate leakage density could cause the final degradation of the AlGaN barrier. [ABSTRACT FROM AUTHOR]

A new superjunction MOSFET (SJ-MOSFET) architecture with dual built-in Schottky diodes is proposed and studied with the numerical TCAD simulations. This letter is based on silicon. One Schottky contact is formed at the top of the n-pillar, while the other is formed at the bottom of the p-pillar. During the reverse conduction period, the Schottky junctions turn on at a lower voltage than the PN junction. The current flows through n-pillar and p-pillar in parallel, so the potential difference across the PN junction is kept below its turn-on voltage. Thus, minority carrier injection through the PN junction is completely suppressed, leading to a superior reverse recovery performance. Integration of a single Schottky contact to either the n-pillar or the p-pillar cannot completely suppress the turn-on of the PN junction in the SJ-MOSFET due to the potential drop created by the current through only one type of the pillars. Furthermore, the proposed dual-Schottky SJ-MOSFET reduces the gate charge (${Q} _{\mathrm {G}}$) and the gate-to-drain charge (${Q} _{\mathrm {GD}}$), compared with the conventional SJ-MOSFET, leading to better figures of merit. [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]

The impacts of static and dynamic gate stress on the threshold voltage (${V}_{\text {TH}}$) instability in Schottky-type ${p}$ -GaN gate AlGaN/GaN heterojunction field-effect transistors are experimentally investigated. ${V}_{\text {TH}}$ shifts negatively under large positive bias static stress (${V}_{\text {G}}\_ {\text {stress}} > 5$ V) by adopting conventional quasi-static characterization techniques. In contrast, ${V}_{\text {TH}}$ under fast-dynamic-stress exhibits positive shift, and a positive frequency dependence occurs within a wide range of frequency from 10 Hz to 1 MHz. The different ${V}_{\text {TH}}$ instability behavior under static and dynamic stress mainly originates from the time-dependent charges (electrons and holes) storage/release mechanisms in the ${p}$ -GaN layer, which is floating in the Schottky-type ${p}$ -GaN gate HEMT. [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]

Effective interface trap characterization approaches are indispensable in the development of gate stack and dielectric surface passivation technologies in III-nitride (III-N) insulated-gate power switching transistors for enhanced stability and dynamic performance. In III-N metal-insulator-semiconductor high-electron-mobility transistors (MIS-HEMTs) that feature a buried channel, the polarized barrier layer separates the critical dielectric/III-N interface from the two-dimensional electron gas (2DEG) channel and consequently complicates interface trap analysis. The barrier layer not only causes underestimation/uncertainty in interface trap extraction using conventional ac-conductance method but also allows the Fermi level dipping deep into the bandgap at the pinch-off of the 2DEG channel. To address these issues, we analyze the frequency/temperature dispersions of the second slope in capacitance-voltage characteristics and develop systematic ac-capacitance techniques to realize interface trap mapping in MIS-HEMTs. The correlation between ac-capacitance and pulse-mode hysteresis measurements show that appropriate gate bias need to be selected in the interface trap characterization of MIS-HEMTs, in order to match the time constant of interface traps at the Fermi level with ac frequency and pulsewidth. [ABSTRACT FROM AUTHOR]

In this work, by using an on-chip integrated Schottky-on-heterojunction light-emitting diode (SoHLED) which is seamlessly integrated with the AlGaN/GaN high electron mobility transistor (HEMT), we studied the effect of on-chip light illumination on the de-trapping processes of electrons from both surface and bulk traps. Surface trapping was generated by applying OFF-state drain bias stress, while bulk trapping was generated by applying positive substrate bias stress. The detrapping processes of surface and/or bulk traps were monitored by measuring the recovery of dynamic on-resistance Ron and/or threshold voltage Vth of the HEMT. The results show that the recovery processes of both dynamic Ron and threshold voltage Vth of the HEMT can be accelerated by the on-chip SoH-LED light illumination, demonstrating the potentiality of on-chip hybrid opto-HEMTs to minimize the influences of traps during dynamic operation of AlGaN/GaN power HEMTs. [ABSTRACT FROM AUTHOR]

In this work, we attempt to reveal the underlying mechanisms of divergent V TH-thermal-stabilities in III-nitride metal-insulator-semiconductor high-electron-mobility transistor (MIS-HEMT) and MOS-Channel-HEMT (MOSC-HEMT). In marked contrast to MOSC-HEMT featuring temperature-independent VTH, MIS-HEMT with the same high-quality gate-dielectric/III-nitride interface and similar interface trap distribution exhibits manifest thermally induced VTH shift. The temperature-dependent VTH of MIS-HEMT is attributed to the polarized III-nitride barrier layer, which spatially separates the critical gate-dielectric/III-nitride interface from the channel and allows "deeper" interface trap levels emerging above the Fermi level at pinch-off. This model is further experimentally validated by distinct VG-driven Fermi level movements at the critical interfaces in MIS-HEMT and MOSC-HEMT. The mechanisms of polarized III-nitride barrier layer in influencing VTH-thermal-stability provide guidelines for the optimization of insulated-gate III-nitride power switching devices. [ABSTRACT FROM AUTHOR]

Al2O3/AlGaN/GaN enhancement-mode metal-isolator-semiconductor high-electron-mobility transistor (MIS-HEMT) featuring a partially recessed (Al) GaN barrier was realized by a fluorine plasma implantation/etch technique. By properly adjusting the RF power driving the fluorine plasma, the fluorine plasma is able to produce two desirable results: 1) a well-controlled slow dry etching for gate recess and 2) implanting fluorine ions into the AlGaN barrier. The fluorine ions become negatively charged in the barrier layer and induce a positive shift in the threshold voltage. The proposed MIS-HEMT exhibits a threshold voltage ( V\mathrm {\mathbf {TH}}) of +0.6 V at a drain current of 10~\mu \textA /mm, a maximum drive current of 730 mA/mm, an ON-resistance of 7.07~\Omega \,\cdot \, mm, and an OFF-state breakdown voltage of 703 V at an OFF-state drain leakage current of 1~\mu \text{A} /mm. From room temperature to 200 °C, the device exhibits a small negative shift of V_{\mathrm {\mathbf {TH}}}$ ( $\sim 0.5$ V) that is attributed to the high-quality dielectric/F-implanted-(Al) GaN interface and the partially recessed barrier. [ABSTRACT FROM AUTHOR]