Analysis reveals carrier trapping and annihilation processes in metal-halide perovskites, indicating operational insights for optoelectronic applications.
Understanding carrier dynamics in photoexcited metal-halide perovskites is key for optoelectronic devices such as solar cells (low carrier densities) and lasers (high carrier densities). Trapping processes at low carrier densities and many-body recombination at high densities can significantly alter the dynamics of photoexcited carriers. Combining optical-pump/THz probe and transient absorption spectroscopy we examine carrier responses over a wide density range (1014-1019 cm-3) and temperatures (78-315 K) in the prototypical methylammonium lead iodide perovskite. At densities below ∼1015 cm-3 (room temperature, sunlight conditions), fast carrier trapping at shallow trap states occurs within a few picoseconds. As excited carrier densities increase, trapping saturates, and the carrier response stabilizes, lasting up to hundreds of picoseconds at densities around ∼1017 cm-3. Above 1018 cm-3 a Mott transition sets in overlapping polaron wave functions leading to ultrafast annihilation, tentatively assigned as an Auger recombination process, occurring over a few picoseconds. We map out trap-dominated, direct recombination-dominated, and Mott-dominated density regimes from 78 to 315 K, ultimately enabling the construction of an electronic "phase diagram". These findings clarify carrier behavior across operational conditions, aiding material optimization for optoelectronics operating in the low (e.g., photovoltaics) and high (e.g., laser) carrier density regimes.
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Wang et al. (2025) studied this question.
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