People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Mosconi, Edoardo
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (34/34 displayed)
- 2024Reaction Mechanism of Hydrogen Generation and Nitrogen Fixation at Carbon Nitride/Double Perovskite Heterojunctionscitations
- 2023Cu/Ag–Sb–I Rudorffite Thin Films for Photovoltaic Applicationscitations
- 2023Band gap tuning through cation and halide alloying in mechanochemically synthesized Cs3(Sb1−xBix)2Br9 and Cs3Sb2(I1−xBrx)9 solid solutionscitations
- 2023Synergistic Role of Water and Oxygen Leads to Degradation in Formamidinium-Based Halide Perovskitescitations
- 2023Plasma‐Driven Atomic‐Scale Tuning of Metal Halide Perovskite Surfaces: Rationale and Photovoltaic Applicationcitations
- 2023Band gap tuning through cation and halide alloying in mechanochemically synthesized Cs<sub>3</sub>(Sb<sub>1−<i>x</i></sub>Bi<sub><i>x</i></sub>)<sub>2</sub>Br<sub>9</sub> and Cs<sub>3</sub>Sb<sub>2</sub>(I<sub>1−<i>x</i></sub>Br<sub><i>x</i></sub>)<sub>9</sub> solid solutionscitations
- 2023Rationalizing Electron–Phonon Interactions and Hot Carriers Cooling in 2D to 3D Metal Halide Perovskitescitations
- 2023Band Gap Tuning Through Cation and Halide Alloying in Mechanochemical Synthesized Cs3(Sb1-xBix)2Br9 and Cs3Sb2(I1-xBrx)9 Solid Solutionscitations
- 2023Air- and water-stable and photocatalytically active germanium-based 2D perovskites by organic spacer engineeringcitations
- 2023Air- and water-stable and photocatalytically active germanium-based 2D perovskites by organic spacer engineeringcitations
- 2022Modification of a Buried Interface with Bulky Organic Cations for Highly Stable Flexible Perovskite Solar Cellscitations
- 2022Reaction Mechanism of Photocatalytic Hydrogen Production at Water/Tin Halide Perovskite Interfacescitations
- 2022Heterovalent Tin Alloying in Layered MA3Sb2I9 Thin Films: Assessing the Origin of Enhanced Absorption and Self-Stabilizing Charge Statescitations
- 2022Understanding performance limiting interfacial recombination in pin Perovskite solar cellscitations
- 2022Defect Formation and Healing at Grain Boundaries in Lead-Halide Perovskitescitations
- 2021Designing New Indene-Fullerene Derivatives as Electron-Transporting Materials for Flexible Perovskite Solar Cellscitations
- 2021Experimental Strategy and Mechanistic View to Boost the Photocatalytic Activity of Cs3Bi2Br9 Lead‐Free Perovskite Derivative by g‐C3N4 Composite Engineeringcitations
- 2021Cation Engineering for Resonant Energy Level Alignment in Two-Dimensional Lead Halide Perovskitescitations
- 2021Water‐Stable DMASnBr3 Lead‐Free Perovskite for Effective Solar‐Driven Photocatalysiscitations
- 2021Outstanding passivation effect by a mixed-salt interlayer with internal interactions in perovskite solar cellscitations
- 2021Water-Stable DMASnBr3 Lead-Free Perovskite for Effective Solar-Driven Photocatalysiscitations
- 2021Ligand-engineered bandgap stability in mixed-halide perovskite LEDscitations
- 2020Comparing the excited-state properties of a mixed-cation–mixed-halide perovskite to methylammonium lead iodidecitations
- 2020Combined computational and experimental investigation on the nature of hydrated iodoplumbate complexes: Insights into the dual role of water in perovskite precursor solutionscitations
- 2020Origin of pressure-induced band gap tuning in tin halide perovskitescitations
- 2020Origin of pressure-induced band gap tuning in tin halide perovskitescitations
- 2019Influence of Disorder and Anharmonic Fluctuations on the Dynamical Rashba Effect in Purely Inorganic Lead-Halide Perovskitescitations
- 2019Charge Carriers Are Not Affected by the Relatively Slow-Rotating Methylammonium Cations in Lead Halide Perovskite Thin Filmscitations
- 2019Charge Carriers Are Not Affected by the Relatively Slow-Rotating Methylammonium Cations in Lead Halide Perovskite Thin Filmscitations
- 2019Controlling competing photochemical reactions stabilizes perovskite solar cellscitations
- 2019Charge Carriers Are Not Affected by the Relatively Slow-Rotating Methylammonium Cations in Lead Halide Perovskite Thin Films.
- 2019Band Gap Engineering in MASnBr3and CsSnBr3 Perovskites: Mechanistic Insights through the Application of Pressurecitations
- 2018Ionotronic halide perovskite drift-diffusive synapses for low-power neuromorphic computationcitations
- 2018Iodine chemistry determines the defect tolerance of lead-halide perovskitescitations
Places of action
Organizations | Location | People |
---|
article
Charge Carriers Are Not Affected by the Relatively Slow-Rotating Methylammonium Cations in Lead Halide Perovskite Thin Films
Abstract
<p>Recently, several studies have investigated dielectric properties as a possible origin of the exceptional optoelectronic properties of metal halide perovskites (MHPs). In this study we investigated the temperature-dependent dielectric behavior of different MHP films at different frequencies. In the gigahertz regime, dielectric losses in methylammonium-based samples are dominated by the rotational dynamics of the organic cation. Upon increasing the temperature from 160 to 300 K, the rotational relaxation time, τ, decreases from 400 (200) to 6 (1) ps for MAPb-I<sub>3</sub> (-Br<sub>3</sub>). By contrast, we found negligible temperature-dependent variations in τ for a mixed cation/mixed halide FA<sub>0.85</sub>MA<sub>0.15</sub>Pb(I<sub>0.85</sub>Br<sub>0.15</sub>)<sub>3</sub>. From temperature-dependent time-resolved microwave conductance measurements we conclude that the dipolar reorientation of the MA cation does not affect charge carrier mobility and lifetime in MHPs. Therefore, charge carriers do not feel the relatively slow-moving MA cations, despite their great impact on the dielectric constants.</p>