air-stability of some compositions has motivated researchers to find lead-free alternatives. [7,8] A wide range of materials classes have recently been explored computationally and experimentally. [8,9] In evaluating the potential of these new materials for photovoltaics, much of the focus has been on the bandgap, stability, absorption coefficient, and phase. [8,[10][11][12][13] The minority-carrier lifetime has received less attention, yet has historically limited the development of new photovoltaic materials. [14,15] However, the reported lifetimes of lead-free alternatives to the perovskites have typically ranged from <0.1 to ≈10 ns. [15][16][17] Silver-bismuth double perovskites (e.g., Cs 2 AgBiBr 6 and Cs 2 AgBiCl 6 ) have recently been found to be an exception. Time-resolved photoluminescence (TRPL) measurements of these materials show an initial drop in photo luminescence (PL) over a nanosecond timescale by 0.5-2 orders of magnitude, followed by a slow tail in PL decay. These PL decay traces are fit with a bi-or triexponential model and the longest time constant is attributed to the fundamental lifetime, which has been found to be ≥100 ns. [18][19][20] Given that these materials have also been found to be more stable than methylammonium lead iodide, [18,20] they have attracted significant interest, with many recent investigations of new families of double perovskite compounds with novel properties.There is current interest in finding nontoxic alternatives to lead-halide perovskites for optoelectronic applications. Silver-bismuth double perovskites have recently gained attention, but evaluating their carrier lifetime and recombination mechanisms from photoluminescence measurements is challenging due to their indirect bandgap. In this work, transient absorption spectroscopy is used to directly track the photocarrier population in Cs 2 AgBiBr 6 by measuring the ground state bleach dynamics. A small initial drop is resolved in the ground state bleach on a picosecond timescale, after which the remaining photocarriers decay monoexponentially with a lifetime of 1.4 µs. The majority of the early-time decay is attributed to hot-carrier thermalization from the direct transition to the indirect bandgap, and the 1.4 µs lifetime represents the recombination of most photocarriers. From this lifetime, a steady-state excess carrier density of 2.2 × 10 16 cm −3 under 1 sun is calculated, which is an order of magnitude larger than that for methylammonium lead iodide, suggesting that charge transport and extraction can be efficient in Cs 2 AgBiBr 6 solar cells.
Double PerovskiteLead-halide perovskites display remarkable optoelectronic properties, with long diffusion lengths >1 µm, [1,2] strong optical absorption on the order of 10 5 cm −1 , [3] and high photoluminescence quantum efficiencies >80%. [4] These properties have led to rapid increases in the efficiency of perovskite solar cells (up to a certified power conversion efficiency of 22.7%) [5] and light emitting diodes (>11% external quantum efficiency) [6] over a sho...