“…At the In 2 O 3 –Au–CdS interface, the Fermi energy level of Au lies lower than that of CdS and In 2 O 3 . The Schottky contact will form between semiconductors and Au NPs, where the electrons jump from the CB of CdS and In 2 O 3 to Au NPs, and the Au NPs work as a cocatalyst in the generation of hydrogen (pathway II). ,,, At the In 2 O 3 –CdS–Au interface, In 2 O 3 , CdS, and Au have intimate contact with each other and form the three inner interfaces of In 2 O 3 –CdS, In 2 O 3 –Au, and CdS–Au where one type-I heterojunction and a couple of Schottky contacts exist at the same time; thus, the photogenerated electrons not only transfer from In 2 O 3 to CdS and Au but also transfer along the In 2 O 3 –Au and CdS–Au interfaces under the driving forces of the double inner electronic field resulting from the heterojunction and Schottky barrier, facilitating the separation of charge carriers (pathway III). Moreover, due to the SPR effect of noble metal, Au NPs absorb visible light to produce the photogenerated hot electrons, resulting in an improvement of charge carrier density. ,, The synergistic effects of the SPR effect, the heterojunction between semiconductor and semiconductor, and the Schottky barrier between semiconductor and noble metal facilitate the utilization of the light source and accelerate the generation and separation of electrons and holes, thus boosting the generation of H 2 .…”