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001 | 874369 | ||
005 | 20210130004647.0 | ||
024 | 7 | _ | |a 2128/24488 |2 Handle |
037 | _ | _ | |a FZJ-2020-01392 |
041 | _ | _ | |a English |
100 | 1 | _ | |a Lechermann, Frank |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
111 | 2 | _ | |a NIC Symposium 2020 |c Jülich |d 2020-02-27 - 2020-02-28 |w Germany |
245 | _ | _ | |a Cooperation of Many-Body Physics and Defect Chemistry in Transition-Metal Oxides |
260 | _ | _ | |a Jülich |c 2020 |b Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag |
295 | 1 | 0 | |a NIC Symposium 2020 |
300 | _ | _ | |a 93 - 100 |
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490 | 0 | _ | |a Publication Series of the John von Neumann Institute for Computing (NIC) NIC Series |v 50 |
520 | _ | _ | |a The problem of defects in correlated materials is at the heart of the fascinating phenomenology of many of these compounds. A vast number of prominent features of strongly correlated systems, such as e. g. high-temperature superconductivity in cuprates and iron pnictides, or heavy-fermion physics in Ce-based compounds is often directly associated with a defect-crystal state. Already the very concept of a doped Mott-insulator builds up on the understanding of impurities implanted in an otherwise perfect crystal lattice. However, a deeper understanding of the realistic physics is then connected to a faithful description of the defect chemistry underlying the material under consideration. We here show that the combination of density functional theory (DFT) with dynamical mean-field theory (DMFT) provides a proper tool to elucidate this realistic interplay between many-body physics and defect chemistry. Focus is on transition-metal oxides which are well known to harbour diverse manifestations of electronic correlations. Two prominent concrete examples, the paramagnetic metal-to-insulator transition in V$_{2}$O$_{3}$ driven by chromium doping, and the long-standing issue of lithium-doped NiO will be addressed in some detail. |
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