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Correlation between Electronic Defect States Distribution and Device Performance of Perovskite Solar Cells

Giovanni LandiDipartimento di Ingegneria Industriale (DIIn) Università di Salerno Via Giovanni Paolo II 132 84084 Fisciano (SA) ItalyH. C. NeitzertDipartimento di Ingegneria Industriale (DIIn) Università di Salerno Via Giovanni Paolo II 132 84084 Fisciano (SA) ItalyC. BaroneDipartimento di Fisica “E.R. Caianiello” and CNR‐SPIN Salerno Università di Salerno Via Giovanni Paolo II 132 84084 Fisciano (SA) ItalyC. MauroDipartimento di Fisica “E.R. Caianiello” and CNR‐SPIN Salerno Università di Salerno Via Giovanni Paolo II 132 84084 Fisciano (SA) ItalyFelix LangHelmholtz‐Zentrum Berlin für Materialien und Energie GmbH Institut für Silizium Photovoltaik Kekuléstr. 5 12489 Berlin GermanySteve AlbrechtHelmholtz‐Zentrum Berlin für Materialien und Energie GmbH Institut für Silizium Photovoltaik Kekuléstr. 5 12489 Berlin GermanyB. RechHelmholtz‐Zentrum Berlin für Materialien und Energie GmbH Institut für Silizium Photovoltaik Kekuléstr. 5 12489 Berlin GermanyS. PaganoDipartimento di Fisica “E.R. Caianiello” and CNR‐SPIN Salerno Università di Salerno Via Giovanni Paolo II 132 84084 Fisciano (SA) Italy
2017en
ABI

Аннотация

Abstract In the present study, random current fluctuations measured at different temperatures and for different illumination levels are used to understand the charge carrier kinetics in methylammonium lead iodide CH 3 NH 3 PbI 3 ‐based perovskite solar cells. A model, combining trapping/detrapping, recombination mechanisms, and electron–phonon scattering, is formulated evidencing how the presence of shallow and deeper band tail states influences the solar cell recombination losses. At low temperatures, the observed cascade capture process indicates that the trapping of the charge carriers by shallow defects is phonon assisted directly followed by their recombination. By increasing the temperature, a phase modification of the CH 3 NH 3 PbI 3 absorber layer occurs and for temperatures above the phase transition at about 160 K the capture of the charge carrier takes place in two steps. The electron is first captured by a shallow defect and then it can be either emitted or thermalize down to a deeper band tail state and recombines subsequently. This result reveals that in perovskite solar cells the recombination kinetics is strongly influenced by the electron–phonon interactions. A clear correlation between the morphological structure of the perovskite grains, the energy disorder of the defect states, and the device performance is demonstrated.

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