Excitons versus free charges in organo-lead tri-halide perovskites

Excitons versus free charges in organo-lead tri-halide perovskites

8 Apr 2014 | Valerio D'Innocenzo¹,²,*, Giulia Grancini¹,*, Marcelo J.P. Alcocer¹,², Ajay Ram Srimath Kandada¹, Samuel D. Stranks³, Michael M. Lee³, Guglielmo Lanzani¹,², Henry J. Snaith³ & Annamaria Petrozza¹
This study investigates the role of excitons versus free charges in organo-lead tri-halide perovskites, focusing on their impact on photovoltaic (PV) performance. Using optical spectroscopy, the researchers estimate the exciton binding energy in mixed-halide perovskite crystals to be around 50 meV. This value is consistent with almost complete ionization of excitons under PV operating conditions. However, at higher photoexcitation densities, excitonic species dominate, suggesting potential for broader optoelectronic applications. Perovskite solar cells were first introduced in a dye-sensitized configuration, where the dye was replaced by organo-lead halide perovskite crystals. The study shows that perovskite absorbers can operate similarly to excitonic absorbers, with comparable performance to the best inorganic thin-film semiconductors. The fundamental question is whether bound excitons are created and transport energy to the heterojunction, or whether free charges are spontaneously generated within the perovskite. The researchers used the temperature dependence of the absorption band edge to estimate the exciton binding energy in mixed-halide perovskite crystals. They applied the Saha equation to estimate the equilibrium branching ratio between free charges and bound excitons as a function of temperature and charge density. The results show that at equilibrium, following photoexcitation, there is a predominant fraction of free charges in the PV operating regime. The study also examines the temperature dependence of optical absorption in perovskite crystals, showing a 'Varshni' trend in the band gap energy with increasing temperature. The exciton binding energy was estimated to be 55 ± 20 meV. The fraction of free charges over the total photoexcitation was modeled, showing that at room temperature, free charges dominate, even at high excitation densities. The study concludes that perovskite solar cells operate primarily through free charges, not excitons, and that the heterojunction's role is to enable selective charge collection rather than to facilitate exciton ionization. This finding has important implications for the design and performance of perovskite solar cells and other optoelectronic devices.This study investigates the role of excitons versus free charges in organo-lead tri-halide perovskites, focusing on their impact on photovoltaic (PV) performance. Using optical spectroscopy, the researchers estimate the exciton binding energy in mixed-halide perovskite crystals to be around 50 meV. This value is consistent with almost complete ionization of excitons under PV operating conditions. However, at higher photoexcitation densities, excitonic species dominate, suggesting potential for broader optoelectronic applications. Perovskite solar cells were first introduced in a dye-sensitized configuration, where the dye was replaced by organo-lead halide perovskite crystals. The study shows that perovskite absorbers can operate similarly to excitonic absorbers, with comparable performance to the best inorganic thin-film semiconductors. The fundamental question is whether bound excitons are created and transport energy to the heterojunction, or whether free charges are spontaneously generated within the perovskite. The researchers used the temperature dependence of the absorption band edge to estimate the exciton binding energy in mixed-halide perovskite crystals. They applied the Saha equation to estimate the equilibrium branching ratio between free charges and bound excitons as a function of temperature and charge density. The results show that at equilibrium, following photoexcitation, there is a predominant fraction of free charges in the PV operating regime. The study also examines the temperature dependence of optical absorption in perovskite crystals, showing a 'Varshni' trend in the band gap energy with increasing temperature. The exciton binding energy was estimated to be 55 ± 20 meV. The fraction of free charges over the total photoexcitation was modeled, showing that at room temperature, free charges dominate, even at high excitation densities. The study concludes that perovskite solar cells operate primarily through free charges, not excitons, and that the heterojunction's role is to enable selective charge collection rather than to facilitate exciton ionization. This finding has important implications for the design and performance of perovskite solar cells and other optoelectronic devices.
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[slides and audio] Excitons versus free charges in organo-lead tri-halide perovskites