We report the deposition of high-quality SiO 2 and SiN x O y layers onto GaN/sapphire templates by photochemical vapor deposition ͑photo-CVD͒. It was found that the 0.845 nm root-mean-square roughness observed from the photo-CVD SiN x O y layer was much smaller than that observed from photo-CVD SiO 2 layer with the same thickness. GaN metal-insulator-semiconductor ͑MIS͒ capacitors with these insulating layers were also fabricated. With an applied electric field of 4 MV/cm, it was found that the leakage current densities were 1 ϫ 10 −8 and 6 ϫ 10 −7 A/cm 2 for the capacitors with photo-CVD SiN x O y and photo-CVD SiO 2 insulating layers, respectively. It was also found that the breakdown field of the capacitors with photo-CVD SiN x O y could reach 13 MV/cm. The interface state density at the SiN x O y /GaN interface was also found to be reasonably low.Gallium nitride ͑GaN͒ possesses excellent physical and electrical properties, such as wide bandgap, high breakdown field, high saturation electron drift velocity, and good thermal stability. These properties make it particularly suitable for applications in high-speed, high-power, and high-frequency electronic devices operating at elevated temperatures. In the past years, GaN-based transistors such as metal-semiconductor field-effect-transistors ͑MES-FETs͒, heterostructure FETs ͑HFETs͒, and high-electron-mobility transistors ͑HEMTs͒ have all been successfully developed. 1-4 However, the performances of these devices were not as good as expected. Because the surface of nitride-based epitaxial layers is defective in general, it is difficult to achieve high-quality Schottky contacts. As a result, gate leakage currents are often large in GaN-based MES-FETs, HFETs, and HEMTs. Gate leakage currents are much smaller in metal-insulator-semiconductor FETs ͑MIS-FETs͒ and MIS-HFETs. Previously, the fabrications of GaN-based MIS-FETs and MISHFETs using Si 3 N 4 , Ga 2 O 3 , Gd 2 O 3 , SiO 2 , MgO, Sc 2 O 3 , and stacked multilayer oxide as the insulating material have all been demonstrated. [5][6][7][8][9][10][11][12][13][14][15] Various techniques, such as plasma-enhanced chemical vapor deposition ͑PECVD͒, electron cyclotron resonance CVD ͑ECR-CVD͒, jet vapor deposition ͑JVD͒, low-pressure chemical vapor deposition ͑LPCVD͒, thermal oxidation, and photoelectrochemical oxidation ͑PEC͒ have all been used to deposit the insulator materials. 5-15 Photochemical vapor deposition ͑photo-CVD͒ system is another tool that can be used to grow high-quality insulators. [16][17][18][19][20][21] In using the photo-CVD system to grow thin films, it is important to select a proper light source with a radiation spectrum matching the absorption spectra of the reactant gases. Figure 1 shows a schematic diagram of our photo-CVD system with a 150 W water-cooled deuterium ͑D 2 ͒ lamp ͑Hamamatsu L1835͒ as the excitation source. This D 2 lamp emits strong UV and vacuum UV ͑VUV͒ light in the spectral region between 115 and 400 nm. Using such a system, we successfully fabricated Al/photo-CVD SiO 2 /GaN MI...