Modeling noncollinear magnetism in manganese oxides
- Datum: 14.05.2018
- Uhrzeit: 11:00
- Vortragende(r): Prof. Andrew Rappe
- University of Pennsylvania, Department of Chemistry, Philadelphia, U.S.A.
- Ort: Max-Planck-Institut für Mikrostrukturphysik, Weinberg 2, 06120 Halle (Saale)
- Raum: New Lecture Hall, Building B
- Gastgeber: Max-Planck-Institut für Mikrostrukturphysik
- Kontakt: email@example.com
Magnetism in oxides is presently the focus of intense research effort, both due to fundamental interest and due to potential applications. Magnetic oxides can enable ultrasensitive sensors, low-power computing, and metal-insulator transitions. In many cases, the magnetism is noncollinear, due either to magnetic frustration, relativistic spin-orbit coupling, or both. This opens up many complicated spin-spin interactions that lead to competing ground states and exotic interactions.
To enable accurate analysis of magnetic interactions in oxides, we revisit the pseudopotential approximation to enhance its ability to reproduce magnetic energetics. We find that DFT+U is not sufficient for differentiating subtle differences in magnetic properties, but that the fully anisotropic DFT+U+J Hamiltonian can be made to be quite accurate, in concert with a pseudopotential that has semicore states and nonlinear core correction. With this improved pseudopotential, a wide range of spin patterns are successfully reproduced in a family of binary manganese oxides.
We use this new pseudopotential to investigate the nature of magnetism and its coupling to electric polarization in quadruple perovskite CaMn7O12. This material has helicoidal magnetic order, stemming from magnetic frustration in the (111) planes and ferromagnetic coupling between Mn3+ and Mn4+ ions. DFT+U+J calculations show that the experimentally-observed helicoidal order is energetically preferred, even in the absence of spin-orbit coupling and without symmetry-breaking ion displacements. This demonstrates that the main driver for the helicoidal order and the electronic ferroelectricity is nonrelativistic exchange striction.