Abstract
Mixed-valence dilanthanide complexes of the type (Cp iPr5) 2Ln 2I 3 (Cp iPr5 = pentaisopropylcyclopentadienyl; Ln = Gd, Tb, Dy) featuring a direct Ln-Ln σ-bonding interaction have been shown to exhibit well-isolated high-spin ground states and, in the case of the Tb and Dy variants, a strong axial magnetic anisotropy that gives rise to a large magnetic coercivity. Here, we report the synthesis and characterization of two new mixed-valence dilanthanide compounds in this series, (Cp iPr5) 2Ln 2I 3 ( 1-Ln; Ln = Ho, Er). Both compounds feature a Ln-Ln bonding interaction, the first such interaction in any molecular compounds of Ho or Er. Like the Tb and Dy congeners, both complexes exhibit high-spin ground states arising from strong spin-spin coupling between the lanthanide 4f electrons and a single σ-type lanthanide-lanthanide bonding electron. Beyond these similarities, however, the magnetic properties of the two compounds diverge. In particular, 1-Er does not exhibit observable magnetic blocking or slow magnetic relaxation, while 1-Ho exhibits magnetic blocking below 28 K, which is the highest temperature among Ho-based single-molecule magnets, and a spin reversal barrier of 556(4) cm -1. Additionally, variable-field magnetization data collected for 1-Ho reveal a coercive field of greater than 32 T below 8 K, more than 6-fold higher than observed for the bulk magnets SmCo 5 and Nd 2Fe 14B, and the highest coercive field reported to date for any single-molecule magnet or molecule-based magnetic material. Multiconfigurational calculations, supported by far-infrared magnetospectroscopy data, reveal that the stark differences in magnetic properties of 1-Ho and 1-Er arise from differences in the local magnetic anisotropy of the lanthanide centers.
Original language | English |
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Pages (from-to) | 18714-18721 |
Number of pages | 8 |
Journal | Journal of the American Chemical Society |
Volume | 146 |
Issue number | 27 |
Early online date | 26 Jun 2024 |
DOIs | |
Publication status | Published - 10 Jul 2024 |
Funding
This research was supported by NSF grant CHE-2102603. Additional support was provided by the Naval Air Warfare Center Weapons Division NISE program (K.R.M. and B.G.H.), ERC grant STG-851504 (J.G.C.K., J.K.S., and N.F.C.), and Royal Society URF191320 (N.F.C.), and Leverhulme Trust RPG-2023-025 (N.F.C.). A portion of this work was performed at the National High Magnetic Field Laboratory, which is supported by National Science Foundation Cooperative Agreement No. DMR-1644779 and DMR-2128556 and the State of Florida. We thank the University of Manchester for access to the Computational Shared Facility, the ILJU Academy and Culture Foundation for support of H.K. through an Overseas Ph.D. Scholarship, and Dr. T. David Harris for discussions and editorial assistance.
Funders | Funder number |
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Engineering Research Centers | STG-851504 |
Royal Society | URF191320 |
National Science Foundation | CHE-2102603, DMR-1644779, DMR-2128556 |
Leverhulme Trust | RPG-2023-025 |