especially in nanostructured forms in order to attain improved system performances. [11,20,26,32] In this regard, ZnO, a transparent semiconducting oxide with a large exciton binding energy (60 meV) and high carrier mobility, has attracted an extensive interest. [5,15,18,[32][33][34] Nevertheless, its performances are detrimentally affected by its wide band gap (E G = 3.3 eV), [3,14,[35][36][37][38][39] limiting radiation absorption to the UV interval (≈5% of the overall solar spectrum), [1,2,38,[40][41][42][43] and by the rapid charge carriers recombination. [33,[35][36][37]44] To tackle these obstacles and extend the system photo response into the vis range, [1,15,39] various investigators have focused on doping with substitutional elements to the Zn and O sites. [3,21,32,40,41,43] Appreciable efforts have also been devoted to the coupling of ZnO with other suitable semiconductors, with the aim of tailoring their interfacial energetics to the targeted photoactivated processes. [2,22,27,36,45,46] In this regard, various heterojunctioncontaining composites based on ZnO-TiO 2 , [8] ZnO-NiO, [31] ZnOCdS, [11] ZnO-CdSe, [34] ZnO-CdTe, [43] ZnO-M(OH) x with M = Co, Ni, [16] ZnO-BiVO 4 , [42] ZnO-WO x coupled with CdSe-CdS, [45] ZnO-ZnS-FeS 2 , [39] and ZnO-CdS-NiO [17] have been developed and tested for solar-driven H 2 O splitting. In this broad scenario, an attractive option involves the use of Fe 2 O 3 and WO 3 as functional activators of ZnO systems for the fabrication of vis-light absorbing photoanodes. In particular, Fe 2 O 3 , an abundant and cheap oxide with a narrow band gap (E G = 2.2 eV), [9,26,28,35] has gained a considerable attention, but its sluggish oxygen evolution kinetics, low carrier lifetime, and short exciton diffusion