ment of CZTSSe is a large open-circuit voltage deficit (V OC,def ). Many optimization strategies borrowed from CIGSSe solar cells have been used to break through the current high V OC,def issue of CZTSSe materials, including isovalent cation doping [5][6][7][8][9][10][11] and gradient band-gap design. [12] Ag is equivalent to Cu but its ion radius is larger than that of Cu, which will reduce the recombination caused by the high density of Cu/Zn antisite defects, thereby reducing V oc,def . [5,13] Simultaneously, Ag doping can enlarge the band gap (E g ) of the absorber layer, which will be effective for increasing the open voltage (V OC ) of thin film photovoltaic devices. [12,[14][15][16][17] Based on the above advantages of Ag doping, our group prepared Ag-doped (Ag,Cu) 2 ZnSnSe 4 solar cells through pre-alloying followed by a selenization process, and the V OC of the devices was improved. [12] There is, however, a problem with incorporating Ag into kesterite film, i.e., Ag diffuses very quickly and easily distributes uniformly throughout the whole absorber film during the high temperature annealing process. Therefore it is difficult to control the content along the depth of CZTSSe films. [14,18] Theoretical calculations and experimental results both show that Ag 2 ZnSn(S,Se) 4 is an n-type material and can form a p-n junction with CZTSSe, [13,15,19] but it cannot ensure the existence of n-type (Cu,Ag) 2 ZnSn(S,Se) 4 on the surface due to the quick diffusion of Ag. So far, surface type As a low-cost substitute that uses no expensive rare-earth elements for the high-efficiency Cu(In,Ga)(S,Se) 2 solar cell, the Cu 2 ZnSn(S,Se) 4 (CZTSSe) solar cell has borrowed optimization strategies used for its predecessor to improve its device performance, including a profiled band gap and surface inversion. Indeed, there have been few reports of constructing CZTSSe absorber layers with surface inversion to improve efficiency. Here, a strategy that designs the CZTSSe absorber to attain surface modification by using n-type Ag 2 ZnSnS 4 is demonstrated. It has been discovered that Ag plays two major roles in the kesterite thin film devices: surface inversion and front gradient distribution. It has not only an excellent carrier transport effect and reduced probability of electron-hole recombination but also results in increased carrier separation by increasing the width of the depletion region, leading to much improved V OC and J SC . Finally, a champion CZTSSe solar cell renders efficiency as high as 12.55%, one of the highest for its type, with the open-circuit voltage deficit reduced to as low as 0.306 V (63.2% Shockley-Queisser limit). The band engineering for surface modification of the absorber and high efficiency achieved here shine a new light on the future of the CZTSSe solar cell.