Abstract

Organic-inorganic halide perovskite solar cells are attracting much attention from the photovoltaic community because of their high conversion efficiencies exceeding 20%. So far, intrinsic superior optoelectronic properties of this material class have been revealed through comprehensive studies on the thin films and single crystals [1,2]. For further improvement of the device architecture and conversion efficiency, the carrier recombination and transport dynamics in actual solar cell devices have to be clarified. The perovskite solar cell is usually implemented as a heterojunction structure consisting of a perovskite absorber layer and charge transport layers as selective contacts, and the carrier-injection properties at these heterointerfaces play a crucial role for the device performance. Time-resolved photoluminescence (PL) techniques are usually adopted to investigate carrier injection and transport properties [3]. However, PL is also additionally affected by traps and defects within the perovskite layer and also at the heterointerface. On the other hand, the photocurrent (PC) measurement can directly assess the net charge-carrier flow through the whole device. Therefore a combination of PL and PC enables us to investigate the details of the carrier injection. In addition, perovskite solar cells are prepared by a fast and cost-effective low-temperature solution-process, but this simple preparation method also causes a spatial nonuniformity in the optical and electrical properties [4]. Thus, the spatial imaging is invaluable for statistical evaluation of the solar cell characteristics.

© 2017 IEEE