The performance of perovskite solar cells is predominantly limited by non-radiative recombination, either through trap-assisted recombination in the absorber layer or via minority carrier recombination at the perovskite/transport layer interfaces. Here, we use transient and absolute photoluminescence imaging to visualize all non-radiative recombination pathways in planar pin-type perovskite solar cells with undoped organic charge transport layers. We find significant quasi-Fermi-level splitting losses (135 meV) in the perovskite bulk, whereas interfacial recombination results in an additional free energy loss of 80 meV at each individual interface, which limits the open-circuit voltage (V) of the complete cell to ~1.12 V. Inserting ultrathi...
With power conversion efficiencies of perovskite-on-silicon and all-perovskite tandem solar cells in...
Nonradiative carrier recombination plays a major role in affecting solar cells’ performance and powe...
© 2020 IUPAC & De Gruyter. This work is licensed under a Creative Commons Attribution-NonCommercia...
The performance of perovskite solar cells is predominantly limited by non radiative recombination, e...
Perovskite solar cells combine high carrier mobilities with long carrier lifetimes and high radiativ...
Charge transport layers (CTLs) are key components of diffusion controlled perovskite solar cells, ho...
With close to 100% internal quantum efficiency over the absorption spectrum, photocurrents in perovs...
Charge transport layers CTLs are key components of diffusion controlled perovskite solar cells, ho...
2D Ruddlesden–Popper perovskite (RPP) solar cells have excellent environmental stability. However, t...
Interface engineering and design is paramount in the optimization of a multilayer device stack. This...
International audienceInterface engineering through passivating agents, in the form of organic molec...
Perovskite semiconductors are an attractive option to overcome the limitations of established silico...
With power conversion efficiencies of perovskite on silicon and all perovskite tandem solar cells in...
Interface engineering and design is paramount in the optimization of a multilayer device stack. This...
With power conversion efficiencies of perovskite-on-silicon and all-perovskite tandem solar cells in...
Nonradiative carrier recombination plays a major role in affecting solar cells’ performance and powe...
© 2020 IUPAC & De Gruyter. This work is licensed under a Creative Commons Attribution-NonCommercia...
The performance of perovskite solar cells is predominantly limited by non radiative recombination, e...
Perovskite solar cells combine high carrier mobilities with long carrier lifetimes and high radiativ...
Charge transport layers (CTLs) are key components of diffusion controlled perovskite solar cells, ho...
With close to 100% internal quantum efficiency over the absorption spectrum, photocurrents in perovs...
Charge transport layers CTLs are key components of diffusion controlled perovskite solar cells, ho...
2D Ruddlesden–Popper perovskite (RPP) solar cells have excellent environmental stability. However, t...
Interface engineering and design is paramount in the optimization of a multilayer device stack. This...
International audienceInterface engineering through passivating agents, in the form of organic molec...
Perovskite semiconductors are an attractive option to overcome the limitations of established silico...
With power conversion efficiencies of perovskite on silicon and all perovskite tandem solar cells in...
Interface engineering and design is paramount in the optimization of a multilayer device stack. This...
With power conversion efficiencies of perovskite-on-silicon and all-perovskite tandem solar cells in...
Nonradiative carrier recombination plays a major role in affecting solar cells’ performance and powe...
© 2020 IUPAC & De Gruyter. This work is licensed under a Creative Commons Attribution-NonCommercia...