This study describes AlGaAs/InGaAs metal-oxide-semiconductor pseudomorphic high-electron-mobility transistors (MOSPHEMTs) with a liquid phase deposited SiO 2 (LPD-SiO 2 ) as the gate dielectric. Compared to its counterpart PHEMT, the AlGaAs/InGaAs MOS-PHEMT exhibits a larger gate bias operation, a higher breakdown voltage, a lower subthreshold current, and an improved gate leakage current with an effectively suppressed impact ionization effect. Consequently, LPD-SiO 2 may also be used as gate oxides and as effective passivation on III-V compound semiconductor devices.InGaAs-channel transistors, such as pseudomorphic highelectronic-mobility transistors (PHEMTs), are useful for achieving enhanced electron mobility. Recent progress in AlGaAs/InGaAs PHEMTs with a low Al-content AlGaAs Schottky layer grown on top of an InGaAs channel has shown promising features and performance in communication systems and for commercial purposes. However, the main issues of Schottky-based devices are limited gate voltage swing, lower breakdown voltage, and higher gate leakage current. Insulators are commonly chosen for growth on the III-V compound semiconductor to fabricate the metal-oxide-semiconductor (MOS) gate with a larger gate swing voltage and lower leakage current. [1][2][3][4] Silicon dioxide (SiO 2 ) is one of the commonly used dielectrics for III-V semiconductor devices. Numerous methods have been used to successfully deposit SiO 2 films, such as low-pressure chemical vapor deposition (LPCVD), 5 plasma-enhanced chemical vapor deposition (PECVD), 6,7 electron cyclotron resonance chemical vapor deposition (ECR-CVD), 8 sputtering, 9 rapid thermal oxidation (RTO), 10 and liquid phase deposition (LPD). 11,12 Compared with other methods, LPD is a low-cost and low-temperature process. In addition, neither anodic equipment nor an assisting energy source is required in the LPD system. Our previous studies have shown LPD-SiO 2 on Si, 13 GaAs, 14 GaN, 15 and AlGaAs. 16 Based on our experiments, however, the LPDSiO 2 method is unsuitable for certain types of semiconductor materials, as shown in Table I, which limits further device applications. In this study, the 1×100 μm 2 AlGaAs/InGaAs MOS-PHEMT with an LPD-SiO 2 as a gate dielectric was fabricated and direct-current (dc) characteristics were discussed.
ExperimentalThe proposed device structures were grown by metal-organic chemical vapor deposition (MOCVD) on a semi-insulating GaAs substrate. The buffer layer consists of 100 nm undoped GaAs, followed by 250 nm undoped Al 0.2 Ga 0.8 As followed by 60 nm GaAs. A 10 nm Al 0.2 Ga 0.8 As with a Si doping density of 4.5 × 10 17 cm −3 and a 2 nm undoped Al 0.2 Ga 0.8 As spacer layer were then grown on the buffer layer, followed by a 14 nm undoped In 0.15 Ga 0.85 As channel layer, a 2 nm undoped Al 0.2 Ga 0.8 As spacer layer, a 18 nm Al 0.2 Ga 0.8 As donor layer with a Si doping density of 1.2×10 18 cm −3 , a 70 nm Al 0.2 Ga 0.8 As Schottky layer with a Si doping density of 1 × 10 17 cm −3 , and a 60 nm GaAs cap layer. Hall measurements sho...