>10 5 cm -1 in the visible light region), [1] a proper bandgap (≈1.5 eV), [2] suitable band edge (valence band maximum: 0.8 eV; conduction band minimum: −0.7 eV, vs NHE), [3] adjustability of structure and properties, [4] and so on. In the past decade, CZTS-based TFSCs have made significant advances in laboratory research. [5] Recently, the certified record conversion efficiency of CZTS-and CZTSSe-based TFSCs have reached 11.0% and 13.0%, respectively. [6] However, these conversion efficiencies are far lower than its theoretical conversion efficiency limit (32.2%). [7] The current research hotspots to improve the conversion efficiency mainly focus on the following two directions: one is the modification of CZTS absorbing materials, and the other is the optimization of device structure of CZTS-based TFSCs. [4] CZTS-based solar cells suffer from low open-circuit voltage (V oc ). The following several factors lead to the low V oc : secondary phases inside the absorber layer and on its boundaries, bandgap fluctuations caused by structural or compositional in-homogeneities, electrostatic potential fluctuations caused by charged defects, and recombination of photogenerated electron-hole pairs via interface states. [8] Compared with other influencing factors, the carrier recombination via interface states is relatively easy to be eliminated through interface engineering. [9] The schematic diagram for device structure of CZTS-based solar cells is shown in Figure 1. The top is window layer containing Al-doped ZnO and intrinsic ZnO (i-ZnO), followed by buffer layer, CZTS absorber layer, Mo back contact and substrate. Among them, the buffer layer plays an important role. The buffer layer is a transition layer between CZTS absorption layer with narrow bandgap and ZnO window layer with wide bandgap. It reduces the bandgap misalignment and lattice mismatch between these two layers, and can prevent the damage to CZTS absorption layer when sputtering ZnO window layer in the process of device fabrication. Furthermore, the buffer layer is also the determinant of the separation and transfer behavior of photogenerated carriers. Therefore, the buffer layer plays an important role in improving the performance of CZTS-based TFSCs. [10] In general, there is a certain potential barrier between the CZTS absorption layer and the carrier transfer layer, which hinders the further improvement of the The current low conversion efficiency of Cu 2 ZnSnS 4 (CZTS)-based thin film solar cells is mainly blamed on the high carrier recombination via interface states at the absorber-buffer. In this work, ZnO 1−x S x solid solution is exploited as the potential buffer layer materials to solve this issue by using density functional theory calculations. With the varying of solid solubility, the lattice constant of ZnO 1−x S x solid solution follows the first-order Vegard's Law, while its bandgap follows the second-order Vegard's Law. Based on the systematical analysis of crystal structure and electronic properties of ZnO 1−x S x solid solution, ZnO 0.375...