Photoinduced Current Transient Spectroscopy on Metal Halide Perovskites: Electron Trapping and Ion Drift AITranslate
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Metal halide perovskites (MHPs) are disruptive materials for a vast class of optoelectronic devices. The presence of electronic trap states has been a tough challenge in terms of characterization and thus mitigation. Many attempts based on electronic spectroscopies have been tested, but due to the mixed electronic–ionic nature of MHP conductivity, many experimental results retain a large ambiguity in resolving electronic and ionic charge contributions. Here we adapt a method, previously used in highly resistive inorganic semiconductors, called photoinduced current transient spectroscopy (PICTS) on lead bromide 2D-like ((PEA)2PbBr4) and standard “3D” (MAPbBr3) MHP single crystals. We present two conceptually different outcomes of the PICTS measurements, distinguishing the different electronic and ionic contributions to the photocurrents based on the different ion drift of the two materials. Our experiments unveil deep level trap states on the 2D, “ion-frozen” (PEA)2PbBr4 and set new boundaries for the applicability of PICTS on 3D MHPs.
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DOI:https://doi.org/10.1021/acsenergylett.3c01429
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Metal halide perovskites (MHPs) are disruptive materials for a vast class of optoelectronic devices. The presence of electronic trap states has been a tough challenge in terms of characterization and thus mitigation. Many attempts based on electronic spectroscopies have been tested, but due to the mixed electronic–ionic nature of MHP conductivity, many experimental results retain a large ambiguity in resolving electronic and ionic charge contributions. Here we adapt a method, previously used in highly resistive inorganic semiconductors, called photoinduced current transient spectroscopy (PICTS) on lead bromide 2D-like ((PEA)2PbBr4) and standard “3D” (MAPbBr3) MHP single crystals. We present two conceptually different outcomes of the PICTS measurements, distinguishing the different electronic and ionic contributions to the photocurrents based on the different ion drift of the two materials. Our experiments unveil deep level trap states on the 2D, “ion-frozen” (PEA)2PbBr4 and set new boundaries for the applicability of PICTS on 3D MHPs.
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| GB/T 7714-2015 | [1] Giovanni Armaroli, Lorenzo Maserati, Andrea Ciavatti, et al. ACS Energy Letters, 2023(8). DOI:10.1021/acsenergylett.3c01429. |
| MLA | [1] Giovanni Armaroli, et al., ACS Energy Letters, no. 8, 2023, https://doi.org/10.1021/acsenergylett.3c01429. |
| APA | [1] Giovanni Armaroli, Lorenzo Maserati, Andrea Ciavatti, Pierpaolo Vecchi, Alberto Piccioni, Martina Foschi, Valentina Van der Meer, Chiara Cortese, Matias Feldman, Vito Foderà, Thibault Lemercier, Julien Zaccaro, Javier Mayén Guillén, Eric GrosDaillon, Beatrice Fraboni, & Daniela Cavalcoli. (2023). ACS Energy Letters(8). https://doi.org/10.1021/acsenergylett.3c01429 |
| IEEE | [1] Giovanni Armaroli, Lorenzo Maserati, Andrea Ciavatti, Pierpaolo Vecchi, Alberto Piccioni, Martina Foschi, Valentina Van der Meer, Chiara Cortese, Matias Feldman, Vito Foderà, Thibault Lemercier, Julien Zaccaro, Javier Mayén Guillén, Eric GrosDaillon, Beatrice Fraboni, and Daniela Cavalcoli, ACS Energy Letters, no. 8, 2023, doi: 10.1021/acsenergylett.3c01429. |
