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Field-Assisted Slow Magnetic Relaxation in a Six-Coordinate Co(II)–Co(III) Complex with Large Negative Anisotropy
61
Citations
55
References
2017
Year
The reaction of Co(CH<sub>3</sub>COO)<sub>2</sub>·4H<sub>2</sub>O with the Schiff base ligand LH<sub>4</sub> derived from o-vanillin and tris(hydroxymethyl)aminomethane produces the dinuclear mixed-valence complex [Co<sup>II</sup>Co<sup>III</sup>(LH<sub>2</sub>)<sub>2</sub>(CH<sub>3</sub>COO)(H<sub>2</sub>O)](H<sub>2</sub>O)<sub>3</sub> (1), which has been investigated using IR spectroscopy, X-ray crystallography, temperature-dependent magnetic susceptibility, magnetization, HFEPR spectroscopy, and ac susceptibility measurements at various frequencies, temperatures, and external magnetic fields. The structure of 1 consists of neutral molecules in which two cobalt ions with distorted octahedral geometries, Co<sup>II</sup>O<sub>6</sub> and Co<sup>III</sup>N<sub>2</sub>O<sub>4</sub>, are bridged by two deprotonated -CH<sub>2</sub>O<sup>-</sup> groups of the two LH<sub>2</sub><sup>2-</sup> ligands. 1 completes a series with Cl, Br, NO<sub>3</sub>, and NCS anions published before by different authors. Low-temperature HFEPR measurements reveal that the ground electronic state of the Co(II) center in 1 is a highly anisotropic Kramers doublet; the effective g values of 7.18, 2.97, and 1.96 are frequency-independent over the frequency ranges 200-630, 200-406, and 200-300 GHz for the highest, intermediate, and lowest g<sub>eff</sub> values, respectively. The two lower values were not seen at higher frequencies because the magnetic field was not high enough. Temperature-dependent magnetic susceptibility and field-dependent magnetization data confirm high magnetic anisotropy of the easy axis type. Complex 1 behaves as a single-ion magnet under a small applied external field and demonstrates two relaxation modes that strongly depend on the applied static dc field. The observation of multiple relaxation pathways clearly distinguishes 1 from the Cl and Br analogues.
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