Compared with the fossil fuels, hydrogen possesses several advantages such as zero carbon emission, versatile production, and high energy density. [1] Solar to hydrogen conversion by photocatalysis is sustainable and renewable without any external power. Therefore, in the past decades numerous efforts have been made to improve photocatalytic hydrogen generation efficiency. For wide bandgap semiconductor materials, they can utilize only a small fraction of solar energy. For example, anatase TiO 2 (E g = 3.2 eV) can only absorb the wavelengths below 388 nm with the theoretical maximum photoconversion efficiency of 1.3% under the AM 1.5 solar spectrum. [2] To improve the photocatalytic hydrogen evolution efficiency, the strategies of energy band engineering by doping, [3,4] solid solution, [5,6] and localized surface plasmon resonance [7,8] have been adopted to achieve bandgap narrowing and visible light absorption. Li et al. [9] reported controllable bandgaps of Zn 1−x Cd x S from 3.10 to 2.30 eV by increasing x from 0 to 1, achieving the visible light photocatalytic hydrogen evolution. Another approach of bandgap engineering is to alloy III-V and II-VI semiconductors. [10] Among all the possible solid solutions, the quaternary GaP-ZnSe, GaP-ZnS, and GaN-ZnO systems exhibit abnormal bandgaps which are smaller than those of the pure component semiconductors. [10] For example, Yang et al. [11] fabricated (GaP) 1−x (ZnSe) x solid-solution nanowires by chemical vapor deposition (CVD). A preferred solubility in the range of x = 0.182-0.209 was obtained, resulting in varied bandgaps of 1.95-2.20. [11] Hart and Allan [12] proposed fabrication of GaP-ZnS solid solution because both GaP and ZnS have the same zinc blende structure. Their calculation indicated that the bandgap of (GaP) 0.875 (ZnS) 0.125 can be reduced to 1.9 eV with a specific ordering of the atoms. This bandgap is lower than those of bare GaP (2.24 eV) and ZnS (3.54 eV). [12] Although the bandgaps of these two solid-solution systems have been brought down to the visible light region, they are not suitable for photocatalytic hydrogen evolution presumably owing to the corrosion susceptibility of GaP. [13] By contrast, the GaN-ZnO system was first experimentally demonstrated to be a promising material for visible-light-driven photocatalytic hydrogen evolution by Domen's group. [5,14,15] Since both GaN and ZnO have a hexagonal close Nanolamination of GaN and ZnO layers by atomic layer deposition (ALD) is employed to fabricate GaN-ZnO homogenous solid-solution thin films because it offers more precise control of the stoichiometry. By varying the ALD cycle ratios of GaN:ZnO from 5:10 to 10:5, the (GaN) 1−x (ZnO) x films with 0.39 ≦ x ≦ 0.79 are obtained. The formation of solid solution is explained based on the atomic stacking and preferred orientation of the layers of GaN and ZnO. However, the growth rates of GaN and ZnO during the lamination process are different from those of pure GaN and ZnO films. It is found that GaN grows faster on ZnO, whereas ZnO grows sl...