Publication date: 11th March 2026
Excess non-radiative recombination is one of the key limitations to further performance improvements in perovskite solar cells[1]. Quantifying and identifying the underlying trap states responsible for recombination is therefore essential for controlling device losses. Recent studies have highlighted that shallow traps dominate recombination in perovskite absorbers, influencing carrier dynamics and device performance[2]. While the theory of deep traps and their impact on frequency-domain response has been investigated, the effect of shallow traps in small-perturbation measurements remains insufficiently understood.
We develop a semi-analytical model that links the trap depth and density to the time constants measured from intensity modulated photovoltage spectroscopy (IMVS). Starting from the Shockley–Read–Hall (SRH) recombination formalism, we derive analytical expressions for the decay time, accounting for both bulk recombination channels and the coupling of the recombination with charge carrier re-injection from the electrodes[3]. The model predicts distinct exponential voltage dependences of the decay time constants, characterized by a slope factor
IMVS measurements performed on devices with different band gaps further validate the model predictions. Slope and ideality factors of 1.5 are frequently observed from electrical measurements, indicating the presence of a high density of deep trap states.
