Abstract
The C3-symmetric crystal-field potential in the Fe(II)Fe(III) bimetallic oxalates splits the L = 2 Fe(II) multiplet into two doublets and one singlet. In compounds that exhibit magnetic compensation, one of the doublets lies lowest in energy and carries an average orbital angular momentum Lzcf that exceeds a threshold value of roughly 0.25. In a range of Lzcf, a Jahn-Teller (JT) distortion enhances the splitting of the low-lying doublet and breaks the C3 symmetry of the bimetallic planes around the ferrimagnetic transition temperature. Due to the competition with the spin-orbit coupling, the JT distortion disappears at low temperatures in compounds that display magnetic compensation. A comparison with recent measurements provides compelling evidence for this inverse, low-temperature JT transition. The size of the JT distortion is estimated using first-principles calculations, which suggest that the long-range ordering of smaller, non-C3-symmetric organic cations can eliminate magnetic compensation.
Original language | English |
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Pages (from-to) | 1740-1745 |
Number of pages | 6 |
Journal | Polyhedron |
Volume | 28 |
Issue number | 9-10 |
DOIs | |
State | Published - Jun 22 2009 |
Funding
We would like to acknowledge conversations with Dr. Murilo Tiago. This research was sponsored by the Laboratory Directed Research and Development Program of Oak Ridge National Laboratory, managed by UT-Battelle, LLC for the US Department of Energy under Contract No. DE-AC05-00OR22725 and by the Division of Materials Science and Engineering of the US DOE.
Funders | Funder number |
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Division of Materials Science and Engineering | |
US Department of Energy | DE-AC05-00OR22725 |
UT-Battelle | |
U.S. Department of Energy | |
Oak Ridge National Laboratory |
Keywords
- Bimetallic oxalates
- Crystal fields
- Jahn-Teller distortion
- Spin-orbit interaction