band gap (E g = 1.0-1.5 eV). [1][2][3][4] Currently, the highest certified power conversion efficiency (PCE) of 13% was obtained for CZTSSe-based thin film solar cell by Xin et al., [5] demonstrating its substantial commercial prospect. While it is still much lower than PCE of the counterpart CIGS devices (23.5%) [6] and its Shockley-Queisser limit (32.8%). [7] There are two main reasons for this. One of the reasons limiting PCE improvement is the complicated defects and defect clusters in CZTSSe, such as Cu Zn , Sn Zn , and 2Cu Zn +Sn Zn , which is resulting from the similar ionic radii and coordination environments of Cu + , Zn 2+ , and Sn 4+ . [8] The presence of harmful deep energy level defects and defect clusters at the bulk of CZTSSe and CZTSSe/CdS interface, resulting in a short minority carrier lifetime and significant band tailing, and hence, a large V OC deficit and low efficiency. In recent years, the most prevalent method to mitigate the defects is equivalent cation substitution, such as Ag substitution for Cu, Cd substitution for Zn, etc. [9,10] Another limitation of PCE is the unfavorable back electrode interface. [11] According to thermodynamic calculations, the Mo/ CZTSSe interface is not as chemically stable as Mo/CIGS interface and the decomposition reaction between CZTSSe absorber and Mo back electrode is inevitable during selenization process, as shown in Equation (1). [12] Thus, the undesired secondary phases are produced at the Mo/CZTSSe back interface, not only damaging the absorber quality but also aggravating the back interface recombination. Meanwhile, the voids would occur at the Mo/ CZTSSe back interface during the decomposition reaction owing to the volatilization of Sn(S,Se) and the diffusion of Cu. The shunt paths caused by these voids reduce the effective volume of the absorber and block the transportation of carrier. [13,14] In addition, it is worth noting that the Mo(S,Se) 2 can form through both the Equations (1) and (2) during selenization process [12,15]