Bulletin of the American Physical Society
APS March Meeting 2020
Volume 65, Number 1
Monday–Friday, March 2–6, 2020; Denver, Colorado
Session D41: Emergent magnetism in correlated electron systems I
2:30 PM–5:30 PM,
Monday, March 2, 2020
Room: 707
Sponsoring
Units:
GMAG DMP DCOMP
Chair: Chetan Dhital, Kennesaw State Univ
Abstract: D41.00005 : The Origin of Ising Magnetism in Ca3Co2O6 Unveiled by Orbital Imaging
Presenter:
Brett Leedahl
(Max Planck Institute for Chemical Physics of Solids)
Authors:
Brett Leedahl
(Max Planck Institute for Chemical Physics of Solids)
Martin Sundermann
(Max Planck Institute for Chemical Physics of Solids)
Andrea Amorese
(Max Planck Institute for Chemical Physics of Solids)
Andrea Severing
(University of Cologne)
Hlynur Gretarsson
(Deutsches Elektronen-Synchrotron (DESY))
Lunyong Zhang
(Max Planck Institute for Chemical Physics of Solids)
Alexander Komarek
(Max Planck Institute for Chemical Physics of Solids)
Antoine Maignan
(Laboratoire CRISMAT)
Maurits Haverkort
(Heidelberg University)
Liu Tjeng
(Max Planck Institute for Chemical Physics of Solids)
One-dimensional CoO6 chains in Ca3Co2O6 arranged in a triangular lattice give rise to an Ising-like magnetism with an intriguing quantum tunneling staircase structure in its magnetization. To resolve the underlying local electronic configuration of the Co ions we applied s-core-level non-resonant inelastic x-ray scattering (s-NIXS), a new technique that is capable of imaging the shape of the 3d orbitals in real space. The orbital shapes that we found established unequivocally that both Co sites (octahedral and trigonal prismatic) are in a 3+ valence state (i.e. 3d6); the trigonal Co site has a high-spin configuration while the octahedral Co site is low spin. Interestingly, we directly ‘see’ that it is the complex d2 orbital that is stabilized by the prismatic trigonal coordination, which naturally explains the Ising magnetism in the system. Utilizing this ability to image electron orbitals, and thus directly relating the orbital occupation with the local crystal structure—without the need for theoretical modeling—is essential for modeling magnetic properties. This is especially true in situations where one would like to make use of the delicate balance of competing interactions to stabilize a particular orbital state for a desired or optimized physical property.
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