2 research outputs found
Modeling Spin Interactions in a Triangular Cobalt(II) Complex with Triaminoguanidine Ligand Framework: Synthesis, Structure, and Magnetic Properties
The
new tritopic triaminoguanidine-based ligand 1,2,3-trisĀ[(pyridine-2-ylmethylidene)Āamino]Āguanidine
(H<sub>2</sub>pytag) was synthesized. The reaction of a mixture of
cobaltĀ(II) chloride and cobaltĀ(II) perchlorate with the ligand H<sub>2</sub>pytag in pyridine solution leads to the formation of the trinuclear
cobaltĀ(II) complex [Co<sub>3</sub>(pytag)Ā(py)<sub>6</sub>Cl<sub>3</sub>]ĀClO<sub>4</sub>. Three octahedrally coordinated high-spin cobaltĀ(II)
ions are linked through the bridging triaminoguanidine backbone of
the ligand leading to an almost equilateral triangular arrangement.
The magnetic properties of the complex were investigated by magnetic
measurements, variable-temperature, variable-field magnetic circular
dichroism (MCD) spectroscopy, and density functional theory as well
as ab initio calculations. A rather strong antiferromagnetic exchange
interaction between the cobaltĀ(II) centers of ca. ā12 cm<sup>ā1</sup> is determined together with a strong local anisotropy.
The single-ion anisotropy of all three cobaltĀ(II) centers is found
to be easy-plane, which coincides with the tritopic ligand plane.
MCD measurements and theoretical investigations demonstrate the presence
of rhombic distortion of the local Co surrounding
A Spin-Frustrated Trinuclear Copper Complex Based on Triaminoguanidine with an Energetically Well-Separated Degenerate Ground State
We
present the synthesis and crystal structure of the trinuclear copper
complex [Cu<sub>3</sub>(saltag)Ā(bpy)<sub>3</sub>]ĀClO<sub>4</sub>Ā·3DMF
[H<sub>5</sub>saltag = trisĀ(2-hydroxybenzylidene)Ātriaminoguanidine;
bpy = 2,2ā²-bipyridine]. The complex crystallizes in the trigonal
space group <i>R</i>3Ģ
, with all copper ions being
crystallographically equivalent. Analysis of the temperature dependence
of the magnetic susceptibility shows that the triaminoguanidine ligand
mediates very strong antiferromagnetic interactions (<i>J</i><sub>CuCu</sub> = ā324 cm<sup>ā1</sup>). Detailed analysis
of the magnetic susceptibility and magnetization data as well as X-band
electron spin resonance spectra, all recorded on both powdered samples
and single crystals, show indications of neither antisymmetric exchange
nor symmetry lowering, thus indicating only a very small splitting
of the degenerate <i>S</i> = <sup>1</sup>/<sub>2</sub> ground
state. These findings are corroborated by density functional theory
calculations, which explain both the strong isotropic and negligible
antisymmetric exchange interactions