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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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Koster, Lja
University of Groningen
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (32/32 displayed)
- 2023The Role of Thermalization in the Cooling Dynamics of Hot Carrier Solar Cellscitations
- 2022A method for identifying the cause of inefficient salt-doping in organic semiconductorscitations
- 2022Vacuum-Deposited Cesium Tin Iodide Thin Films with Tunable Thermoelectric Propertiescitations
- 2022Backbone-driven host-dopant miscibility modulates molecular doping in NDI conjugated polymerscitations
- 2021Amphipathic Side Chain of a Conjugated Polymer Optimizes Dopant Location toward Efficient N-Type Organic Thermoelectricscitations
- 2021Revealing Charge Carrier Mobility and Defect Densities in Metal Halide Perovskites via Space-Charge-Limited Current Measurementscitations
- 2021Understanding Dark Current-Voltage Characteristics in Metal-Halide Perovskite Single Crystalscitations
- 2021Carrier-carrier Coulomb interactions reduce power factor in organic thermoelectricscitations
- 2021Molecular Doping Directed by a Neutral Radicalcitations
- 2020Reaching a Double-Digit Dielectric Constant with Fullerene Derivativescitations
- 2020Electrical Conductivity of Doped Organic Semiconductors Limited by Carrier-Carrier Interactionscitations
- 2020N-type organic thermoelectricscitations
- 2020Toward Understanding Space-Charge Limited Current Measurements on Metal Halide Perovskitescitations
- 20191,8-diiodooctane acts as a photo-acid in organic solar cellscitations
- 2018Enhanced n-Doping Efficiency of a Naphthalenediimide-Based Copolymer through Polar Side Chains for Organic Thermoelectricscitations
- 2017N-Type Organic Thermoelectricscitations
- 2017Relating polymer chemical structure to the stability of polymer:citations
- 2016Deposition of LiF onto Films of Fullerene Derivatives Leads to Bulk Dopingcitations
- 2016N-type polymers as electron extraction layers in hybrid perovskite solar cells with improved ambient stabilitycitations
- 2016A New Figure of Merit for Organic Solar Cells with Transport-limited Photocurrentscitations
- 2016Compatibility of PTB7 and [70]PCBM as a Key Factor for the Stability of PTB7citations
- 2015The Effect of Large Compositional Inhomogeneities on the Performance of Organic Solar Cellscitations
- 2015Strategy for Enhancing the Dielectric Constant of Organic Semiconductors Without Sacrificing Charge Carrier Mobility and Solubilitycitations
- 2014Strategy for Enhancing the Electric Permittivity of Organic Semiconductors
- 2014Charge transport and recombination in PDPP5Tcitations
- 2011Validity of the Einstein Relation in Disordered Organic Semiconductorscitations
- 2007Device physics of polymercitations
- 2007Device physics of donor/acceptor-blend solar cells
- 2007Hybrid polymer solar cells from highly reactive diethylzinccitations
- 2006Light intensity dependence of open-circuit voltage and short-circuit current of polymer/fullerene solar cellscitations
- 2005Origin of the light intensity dependence of the short-circuit current of polymer/fullerene solar cellscitations
- 2004Effect of metal electrodes on the performance of polymercitations
Places of action
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article
The Role of Thermalization in the Cooling Dynamics of Hot Carrier Solar Cells
Abstract
The hot carrier solar cell (HCSC) concept has been proposed to overcome the Shockley Queisser limit of a single p–n junction solar cell by harvesting carriers before they have lost their surplus energy. A promising family of materials for these purposes is metal halide perovskites (MHP). MHPs have experimentally shown very long cooling times, the key requirement of a HCSC. By using ensemble Monte Carlo simulations, light is shed on why cooling times are found to be extended. This article concentrates on the role of thermalization in the cooling process. The role of carrier–phonon and carrier–carrier interactions in thermalization and cooling is specified, while showing how these processes depend on material parameters, such as the dielectric constant and effective mass. It is quantified how thermalization acts as a cooling mechanism via the cold background effect. The importance of a low degree of background doping is to achieve the observed extended cooling times. Herein, it is mapped out how perovskites should be tuned, their material parameters, carrier concentration, and purity, in order to realize a HCSC. It contributes to the debate on the cooling times in MHPs and the suitability of tin perovskites for HCSCs.