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Ultralow dark current in near-infrared perovskite photodiodes by reducing charge injection and interfacial charge generation

Metal halide perovskite photodiodes (PPDs) offer high responsivity and broad spectral sensitivity, making them attractive for low-cost visible and near-infrared sensing. A significant challenge in achieving high detectivity in PPDs is lowering the dark current density (J(D)) and noise current (i(n))...

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Detalles Bibliográficos
Autores principales: Ollearo, Riccardo, Wang, Junke, Dyson, Matthew J., Weijtens, Christ H. L., Fattori, Marco, van Gorkom, Bas T., van Breemen, Albert J. J. M., Meskers, Stefan C. J., Janssen, René A. J., Gelinck, Gerwin H.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8671406/
https://www.ncbi.nlm.nih.gov/pubmed/34907190
http://dx.doi.org/10.1038/s41467-021-27565-1
Descripción
Sumario:Metal halide perovskite photodiodes (PPDs) offer high responsivity and broad spectral sensitivity, making them attractive for low-cost visible and near-infrared sensing. A significant challenge in achieving high detectivity in PPDs is lowering the dark current density (J(D)) and noise current (i(n)). This is commonly accomplished using charge-blocking layers to reduce charge injection. By analyzing the temperature dependence of J(D) for lead-tin based PPDs with different bandgaps and electron-blocking layers (EBL), we demonstrate that while EBLs eliminate electron injection, they facilitate undesired thermal charge generation at the EBL-perovskite interface. The interfacial energy offset between the EBL and the perovskite determines the magnitude and activation energy of J(D). By increasing this offset we realized a PPD with ultralow J(D) and i(n) of 5 × 10(−8) mA cm(−2) and 2 × 10(−14) A Hz(−1/2), respectively, and wavelength sensitivity up to 1050 nm, establishing a new design principle to maximize detectivity in perovskite photodiodes.