Publication | Closed Access
Magnetic Anisotropy in Pentacoordinate Ni<sup>II</sup> and Co<sup>II</sup> Complexes: Unraveling Electronic and Geometrical Contributions
57
Citations
49
References
2016
Year
The magnetic properties of the pentacoordinate [M<sup>II</sup> (Me<sub>4</sub> cyclam)N<sub>3</sub> ]<sup>+</sup> (Me<sub>4</sub> cyclam=tetramethylcyclam; N<sub>3</sub> =azido; M=Ni, Co) complexes were investigated. Magnetization and EPR studies indicate that they have an easy plane of magnetization with axial anisotropy parameters D close to 22 and greater than 30 cm<sup>-1</sup> for the Ni and Co complexes, respectively. Ab initio calculations reproduced the experimental values of the zero-field splitting parameters and allowed the orientation of the anisotropy tensor axes with respect to the molecular frame to be determined. For M=Ni, the principal anisotropy axis lies along the Ni-N<sub>azido</sub> direction perpendicular to the Ni(Me<sub>4</sub> cyclam) mean plane, whereas for M=Co it lies in the Co(Me<sub>4</sub> cyclam) mean plane and thus perpendicular to the Co-N<sub>azido</sub> direction. These orientations match one of the possible solutions experimentally provided by single-crystal cantilever torque magnetometry. To rationalize the geometry and its impact on the orientation of the anisotropy tensor axis, calculations were carried out on model complexes [Ni<sup>II</sup> (NCH)<sub>5</sub> ]<sup>2+</sup> and [Co<sup>II</sup> (NCH)<sub>5</sub> ]<sup>2+</sup> by varying the geometry between square pyramidal and trigonal bipyramidal. The geometry of the complexes was found to be the result of a compromise between the electronic configuration of the metal ion and the structure-orienting effect of the Me<sub>4</sub> cyclam macrocycle. Moreover, the orientation of the anisotropy axes is mainly dependent on the geometry of the complexes.
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