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Activation Energy of Organic Cation Rotation in CH(3)NH(3)PbI(3) and CD(3)NH(3)PbI(3): Quasi-Elastic Neutron Scattering Measurements and First-Principles Analysis Including Nuclear Quantum Effects

[Image: see text] The motion of CH(3)NH(3)(+) cations in the low-temperature phase of the promising photovoltaic material methylammonium lead triiodide (CH(3)NH(3)PbI(3)) is investigated experimentally as well as theoretically, with a particular focus on the activation energy. Inelastic and quasi-el...

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Detalles Bibliográficos
Autores principales: Li, Jingrui, Bouchard, Mathilde, Reiss, Peter, Aldakov, Dmitry, Pouget, Stéphanie, Demadrille, Renaud, Aumaitre, Cyril, Frick, Bernhard, Djurado, David, Rossi, Mariana, Rinke, Patrick
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2018
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6203185/
https://www.ncbi.nlm.nih.gov/pubmed/29961330
http://dx.doi.org/10.1021/acs.jpclett.8b01321
Descripción
Sumario:[Image: see text] The motion of CH(3)NH(3)(+) cations in the low-temperature phase of the promising photovoltaic material methylammonium lead triiodide (CH(3)NH(3)PbI(3)) is investigated experimentally as well as theoretically, with a particular focus on the activation energy. Inelastic and quasi-elastic neutron scattering measurements reveal an activation energy of ∼48 meV. Through a combination of experiments and first-principles calculations, we attribute this activation energy to the relative rotation of CH(3) against an NH(3) group that stays bound to the inorganic cage. The inclusion of nuclear quantum effects through path integral molecular dynamics gives an activation energy of ∼42 meV, in good agreement with the neutron scattering experiments. For deuterated samples (CD(3)NH(3)PbI(3)), both theory and experiment observe a higher activation energy for the rotation of CD(3) against NH(3), which results from the smaller nuclear quantum effects in CD(3). The rotation of the NH(3) group, which is bound to the inorganic cage via strong hydrogen bonding, is unlikely to occur at low temperatures due to its high energy barrier of ∼120 meV.