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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Zu, Fengshuo
Humboldt-Universität zu Berlin
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (18/18 displayed)
- 2024Ion-induced field screening as a dominant factor in perovskite solar cell operational stabilitycitations
- 2023Effect of ground state charge transfer and photoinduced charge separation on the energy level alignment at metal halide perovskite/organic charge transport layer interfaces
- 2023Charge Selective Contacts to Metal Halide Perovskites Studied with Photoelectron Spectroscopy ; X-Ray, Ultraviolet, and Visible Light Induced Energy Level Realignment
- 2022Illumination-Driven Energy Level Realignment at Buried Interfaces between Organic Charge Transport Layers and a Lead Halide Perovskite
- 2022The Electronic Properties of a 2D Ruddlesden‐Popper Perovskite and its Energy Level Alignment with a 3D Perovskite Enable Interfacial Energy Transfercitations
- 2022Electronic properties of metal halide perovskites and their interfaces: the basics
- 2022Understanding performance limiting interfacial recombination in pin Perovskite solar cellscitations
- 2021Mechanism and Timescales of Reversible p‐Doping of Methylammonium Lead Triiodide by Oxygencitations
- 2021Mechanism and Timescales of Reversible p‐Doping of Methylammonium Lead Triiodide by Oxygencitations
- 2021Understanding and suppressing non-radiative losses in methylammonium-free wide-bandgap perovskite solar cellscitations
- 2021Photoinduced energy-level realignment at interfaces between organic semiconductors and metal-halide perovskitescitations
- 2021Reversible oxygen-induced p-doping of mixed-cation halide perovskites
- 2019Constructing the Electronic Structure of CH3NH3PbI3 and CH3NH3PbBr3 Perovskite Thin Films from Single-Crystal Band Structure Measurementscitations
- 2019Unraveling the Electronic Properties of Lead Halide Perovskites with Surface Photovoltage in Photoemission Studiescitations
- 2019The impact of energy alignment and interfacial recombination on the internal and external open-circuit voltage of perovskite solar cellscitations
- 2019High open circuit voltages in pin-type perovskite solar cells through strontium additioncitations
- 2018Interface Engineering of Solution-Processed Hybrid Organohalide Perovskite Solar Cellscitations
- 2017Reduced Interface-Mediated Recombination for High Open-Circuit Voltages in CH3NH3PbI3 Solar Cellscitations
Places of action
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article
Mechanism and Timescales of Reversible p‐Doping of Methylammonium Lead Triiodide by Oxygen
Abstract
<jats:title>Abstract</jats:title><jats:p>Understanding and controlling the energy level alignment at interfaces with metal halide perovskites (MHPs) is essential for realizing the full potential of these materials for use in optoelectronic devices. To date, however, the basic electronic properties of MHPs are still under debate. Particularly, reported Fermi level positions in the energy gap vary from indicating strong n‐ to strong p‐type character for nominally identical materials, raising serious questions about intrinsic and extrinsic defects as dopants. In this work, photoemission experiments demonstrate that thin films of the prototypical methylammonium lead triiodide (MAPbI<jats:sub>3</jats:sub>) behave like an intrinsic semiconductor in the absence of oxygen. Oxygen is then shown to be able to reversibly diffuse into and out of the MAPbI<jats:sub>3</jats:sub> bulk, requiring rather long saturation timescales of ≈1 h (in: ambient air) and over 10 h (out: ultrahigh vacuum), for few 100 nm thick films. Oxygen in the bulk leads to pronounced p‐doping, positioning the Fermi level universally ≈0.55 eV above the valence band maximum. The key doping mechanism is suggested to be molecular oxygen substitution of iodine vacancies, supported by density functional theory calculations. This insight rationalizes previous and future electronic property studies of MHPs and calls for meticulous oxygen exposure protocols.</jats:p>