Defect photophysics of metal-halide pero
Filippo De Angelis a b
a Computational Laboratory for Hybrid/Organic Photovoltaics (CLHYO), CNR-ISTM, Perugia, Italy
b CompuNet, Istituto Italiano di Tecnologia (IIT), Genova, Genova, Italy
Materials for Sustainable Development Conference (MATSUS)
Proceedings of nanoGe Fall Meeting 2018 (NFM18)
Torremolinos, Spain, 2018 October 22nd - 26th
Organizers: Shannon Boettcher, Christophe Delerue, David Egger, Laura Herz, Wolfram Jaegermann, Bernhard Kaiser, Joaquim Puigdollers, Daniel Vanmaekelbergh, Rubén D. Costa, Zeger Hens, Arjan Houtepen, Sandrine Ithurria, Tianquan Lian, Alejandro Perez-Rodriguez, Sascha Sadewasser, Kevin Sivula, Tze-Chien Sum, Alison Walker, Rüdiger Berger, Mischa Bonn, Christian Klinke, Claudio Quarti, Juan J Vilatela and Freddy Rabouw
Invited Speaker, Filippo De Angelis, presentation 339
DOI: https://doi.org/10.29363/nanoge.nfm.2018.339
Publication date: 6th July 2018

The relatively weak bond of metal-halide perovskites  (MHPs) gives rise to an inherently soft crystal lattice which is naturally prone to disorder, [1] associated to formation of defects. Defects introducing levels in the material’s band-gap may act as traps and recombination centers for photogenerated charge carriers, limiting the device performance and possibly impacting the device temporal stability. Defects may also introduce ionic mobility channels in MHPs. Ion migration is boosted by the presence of vacancies and interstitial defects, acting as shuttles for ion hopping.[2] If the migrating defects are also charge traps, as it occurs for iodine defects in MAPbI3, one has migrating traps which can respond to the action of an electric field [3] and to the presence of photogenerated carriers.[4, 5] Some of the traps may also undergo photochemical reactions, such as the reported release of molecular iodine under light irradiation[6, 7]. Defects may also lay behind the reported material transformation under light exposure, followed by very slow relaxation to initial conditions.[8,9]

Theoretical and computational modeling is a complementary tool for rationalizing experimental results, on the one hand, and to direct experiments and device fabrication towards innovative concepts, on the other hand.  Several computational studies have already been carried out on native defects in MHPs, employing Density Functional Theory. The complex interplay of electronic structure and dynamical features of MHPs, however, poses challenging problems to the accuracy and reproducibility of these calculations.[10] Here we present what we believe are the “best practices” in defect modeling of metal-halide perovskites with selected examples of applications related to the effect of electric fields and charge carriers on the structural and electronic properties of perovskites relevant to stability and solar cell operation.

References:

[1] Conings, B. et al. Adv. Energy Mater. 2015, 5, 1500477.

[2] Mosconi, E.; De Angelis, F. ACS Energy Lett. 2016, 1, 182-188.

[3] Chen, B. et al. Nat. Mater., 2018, in press.

[4] Birkhold, S.T.  et al. ACS Energy Lett. 2018, 3, 1279−1286

[5] Meggiolaro, D. et al. Energy Environ. Sci. 2018, 11, 702-713.

[6] Meggiolaro, D. et al. ACS Energy Lett., 2018, 3, 447–451.

[7] Kim, G.Y. et al. Nat Mater 2018, 17, 445-449.

[8] Gottesman, R. et al.  J. Phys. Chem. Lett. 2014, 5, 2662-2669.

[9] Tsai, H. et al. Science 2018, 360, 67-70.

[10] Meggiolaro, D.; De Angelis, F. ACS Energy Lett. 2018, 2206-2222.

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