The artificial photosynthesis of hydrocarbon fuels by photocatalysts is a green and sustainable energy regeneration process, which is essential for environmental protection. [1,2] However, so far, the efficiency of CO 2 photoreduction is relatively low compared with that of photocatalytic H 2 production and contaminants removal degradation. [3][4][5][6] On one hand, the recombination of photogenerated charges inside the semiconductor and on the surface is serious, leading to the severe loss of photogenerated carriers. [7][8][9][10][11][12][13] On the other hand, CO 2 molecules are thermodynamically stable. [14,15] Therefore, a high energy barrier needs to be overcome to activate and hydrogenate CO 2 molecules, which requires robust reductive ability of the photocatalyst. [16] Meanwhile, the protons come from water oxidation; a robust oxidative ability is demanded. [17] S-scheme heterojunction photocatalyst promotes charge separation and maintains enough redox ability. [18][19][20][21][22][23][24][25] In this backdrop, it is feasible to fabricate S-scheme photocatalysts to improve the efficiency of CO 2 photoreduction. [15,26,27] Nevertheless, up to now, most of the S-scheme photocatalysts were achieved by two n-type semiconductors. [10,[28][29][30][31][32][33][34][35][36][37] Therefore, to fully understand the advantages of the S-scheme heterojunction and further improve CO 2 photoreduction activity, this gap needs to be filled.BiOBr, a p-type semiconductor, possesses appropriate conduction band (CB) and valence band (VB) positions, which becomes a promising candidate in our study. [38][39][40] Meanwhile, intense inherent polarization is derived from its layered structure with alternate Br and Bi-O layers. Therefore, a spontaneous internal electrical field (IEF) is formed and favorable for charge separation. [41][42][43][44] Therefore, BiOBr exhibits excellent CO 2 photoreduction performance by the cooperative effect of appropriate band structure and innate IEF. [42] However, low specific surface area, poor CO 2 adsorption ability, and weak reductive capability of BiOBr result in sluggish kinetics of CO 2 photoreduction. [45][46][47] Therefore, an S-scheme heterojunction is needed to couple BiOBr with another semiconductor. [48] NiO is a standard p-type semiconductor with strong reductive ability, which is widely applied in heavy metal reduction, [49] photocatalytic hydrogen production, [50][51][52] CO 2 photoreduction, [53] and photocatalytic overall water splitting. [54,55] An intrinsic NiO semiconductor possesses a wide bandgap of about 4 eV in theory. [56] In practice, synthesized NiO is a p-type semiconductor because of massive Ni vacancies, especially when heated at high temperatures. [51] These Ni vacancies not only narrow the bandgap but also improve the visible light absorption of NiO. [57] Yazdani et al. found that the bandgap of NiO varied from 3.35 to 1.55 eV with the change in annealing temperature. [58] On the contrary, flake morphologies are typical structures for nickel oxides or hydroxides, which...