Semitransparent solar cells have attractedincreasing attention because of their gen eral applications in smart windows for automobiles and buildings, tandem solar cells, electronic chargers, and so on. [1][2][3] Due to facile solution processing and high record efficiency of 23.3% in nontrans parent devices, [4][5][6][7][8] organic-inorganic lead halide perovskite solar cells (PSCs) are excellent candidates for semitransparent devices, since the efficiency of semi transparent devices is inevitably lower compared to devices with fully reflective electrodes. In a typical semitransparent PSC structure, the rear transparent elec trode (RTE) is one of the key components because it is deposited on the underlying soft active layer. So far, various trans parent conductive electrodes have been investigated as RTEs for semitransparent PSCs, such as transparent conductive oxides, [9] conductive polymers, [10] carbon nanotubes, [11] graphene, [12] metal nano wires, [13,14] metal mesh, [15] ultrathin metal films, [16] and so on. Among them, the ultrathin metal films with the thickness below 10 nm have the advantage in the facile deposition pro cess, as well as low sheet resistance, high optical transmittance, and good adhesive strength comparable to other alternatives.The ultrathin silver film exhibits great potential as a low cost, effective RTE material in semitransparent devices. [17][18][19][20] However, there are still some challenges for the application of ultrathin silver films in high performance semitransparent PSCs. First, the 3D growth mode of silver results in separate islands for film thickness below 10 nm, [21] which leads not only low conductivity due to disconnect between parts of the electrode, [22] but also optical loss due to surface plasmonic effect. [23] The smooth and crossconnecting surface morphology of ultrathin silver film is necessary to realize high performance semitransparent PSCs. Second, the band level offset at the silver electrode interface always affects the carrier transport and collection, [24] especially for ultrathin silver electrodes. [25] The chemical interaction at the interface also determines the adhesive strength between silver film and the underlayer, as well as electrode degradation by halide anions and ambientAlthough it exhibits great potential as the rear transparent electrode (RTE) material in semitransparent devices, the ultrathin silver film still faces some significant challenges, such as surface plasmonic effect induced optical loss, the conflict between conductivity and transmittance, and the band level mismatch at device interfaces. In this work, a novel combination of ZrAcac/PEI/Ag/Ta 2 O 5 is employed as the RTE of the semitransparent perovskite solar cells in the planar inverted device structure of "indium-tin-oxide (ITO)/NiO x /MAPbI 3 /PC 61 BM/ZrAcac/PEI/Ag/Ta 2 O 5 ." Interface engineering with ZrAcac/PEI enables a significant increase in the device efficiency for 100 nm thick Ag electrode, from 17.48% to 18.84%. Ultrathin 9 nm Ag film coated on polyetherimide (PE...