Dimension-Controlled Synthesis of Hybrid-Mixed Halide Perovskites for Solar Cell Application

Abstract

Despite the rapid improvement of photovoltaic (PV) efficiency in hybrid organic−inorganic metal halide perovskites (HOIPs), the fabrication procedure of a compact thin film in a large-area application is still a tedious work. Apart from the quality of the thin film, the stability of the perovskite materials and the expensive organic hole transport layer (HTL) within the HOIP-based PV device are the major issues that need to be addressed prior to their commercialization. Herein, a unique glass rod-based facile fabrication technique for producing a compact and stable thin film utilizing a mixed-halide-based perovskite precursor solution is demonstrated. The fabricated devices deliver high photoconversion efficiency (PCE) without the use of any HTL and show an excellent stability under ambient conditions. By varying the organic CH 3 NH 3 I (MAI) and inorganic PbBr 2 content, perovskite materials with different dimensions, i.e., 3D, 2D, and 1D, are synthesized to produce an active layer for PV devices. Although a 2D single-halide perovskite is reported earlier, herein two different mixed-halide 2D perovskites, i.e., MA 2 PbI 2 Br 2 and MAPb 2 IBr 4 , are synthesized successfully, and their performance is compared in detail along with that of 1D and 3D mixed-halide perovskites. The facile synthesized mixed-halide 2D-based MA 2 PbI 2 Br 2 perovskite shows a PCE of 10.14% with a high stability of 92% after 100 days without encapsulation, which is much superior as compared to that of the mixed-halide 3D MAPbIBr 2 . The semiconducting behavior as well as the nature of the bandgap of the synthesized compounds is examined by pursuing density functional theory calculations. Specifically, the role of iodine doping to modify the electronic band structure is investigated, and introduction of iodine is found to reduce the effective masses of both electrons and holes in the perovskite material.

Low-temperature processed additive-incorporated CsPbIBr2-based inverted perovskite solar cells

“…In general, R s originates from the presence of external contacts and accumulation/depletion of charge carriers at the electrode interface. 65 The reduction in R s value upon increasing the additive amount confirms the depletion of the charge carrier at the CuI/perovskite interface, which eventually affects the charge carrier recombination dynamics. From the Nyquist parameters (Table 2), the charge carrier transfer lifetime ( τ tr ) is calculated using the τ = RC equation.…”