“…It is worth mentioning that Mn-Ln complexes containing only Mn(II) ions are quite uncommon compared to Mn(III)-Ln(III) and Mn(III)/Mn(II)-Ln(III) counterparts. 12 The aim of this work is threefold: (i) To establish magneto-structural correlations for the simple Mn(II)Gd(III) dinuclear complexes; (ii) To analyze how magnetothermal properties of this family of closely related Mn(II)Gd(III) based compounds are influenced by the magnitude and sign of the magnetic exchange coupling and (iii) To know if the large anisotropy of the Dy(III) ions, together with the coupling to paramagnetic isotropic Mn(II) ions, could lead to the presence of SMM behaviour in the Dy(III) derivatives.…”
A family of Mn(II)Ln(III) dinuclear and tetranuclear complexes (Ln = Gd and Dy) has been prepared from the compartmental ligands N,N’-dimethyl-N,N’-bis(2-hydroxy-3-formyl-5-bromobenzyl)ethylenediamine (H2L1) and N,N’,N”-trimethyl-N,N”-bis(2-hydroxy-3-methoxy-5-methylbenzyl)diethylenetriamine (H2L2). The Mn(II)Gd(III) complexes exhibit antiferromagnetic...
“…It is worth mentioning that Mn-Ln complexes containing only Mn(II) ions are quite uncommon compared to Mn(III)-Ln(III) and Mn(III)/Mn(II)-Ln(III) counterparts. 12 The aim of this work is threefold: (i) To establish magneto-structural correlations for the simple Mn(II)Gd(III) dinuclear complexes; (ii) To analyze how magnetothermal properties of this family of closely related Mn(II)Gd(III) based compounds are influenced by the magnitude and sign of the magnetic exchange coupling and (iii) To know if the large anisotropy of the Dy(III) ions, together with the coupling to paramagnetic isotropic Mn(II) ions, could lead to the presence of SMM behaviour in the Dy(III) derivatives.…”
A family of Mn(II)Ln(III) dinuclear and tetranuclear complexes (Ln = Gd and Dy) has been prepared from the compartmental ligands N,N’-dimethyl-N,N’-bis(2-hydroxy-3-formyl-5-bromobenzyl)ethylenediamine (H2L1) and N,N’,N”-trimethyl-N,N”-bis(2-hydroxy-3-methoxy-5-methylbenzyl)diethylenetriamine (H2L2). The Mn(II)Gd(III) complexes exhibit antiferromagnetic...
“…The DFT computed spin density suggests dominant spin delocalization on the Co(II) centers with the spin density of 2.749 (Figure d and Figure S11), and the singly occupied π* s -tetrazine radical orbital is energetically close to the Co(II) 3d orbitals . Furthermore, the overlap integral (| S ab |) calculations by using the singly occupied ligand and metal-based molecular orbitals , demonstrated that out of the three possible Co(II)–radical ( s -tetrazine) interactions one of the interactions is really strong (Co(d xy )|p|Rad(π*) = 0.218, Figure e and Figure S12), dominating the strong AF interaction. It should be mentioned that both the DFT and ab initio calculations suggest the presence of small AF interaction between the Co(II) ions, as stated previously in several related complexes .…”
The recent years have witnessed the glory development for the construction of high-performance mononuclear single molecule magnets (SMMs) within a specific coordination geometry, which, however, is not well applied in cluster-based SMMs due to the synthetic challenges. Given that the monocobalt-(II) complexes within a trigonal-prismatic (TPR) coordination geometry have been classified as excellent SMMs with huge axial anisotropy (D ≈ −100 cm −1 ), here we designed and synthesized a new dual-capping tetrazine ligand, 3,6-bis(6-(di(1Hpyrazol-1-yl)methyl)pyridin-2-yl)-1,2,4,5-tetrazine (bpptz), and prepared a novelIn the structure of 1, the bpptz •− radical ligand enwraps two Co(II) centers within quasi-TPR geometries, which are further bridged by the tetrazine radical in the trans mode. The magnetic study revealed that the interaction between the Co centers and the tetrazine radical is strongly antiferromagnetic with a coupling constant (J) of −65.8 cm −1 (in the −2J formalism). Remarkably, 1 exhibited the typical SMM behavior with an effective energy barrier of 69 cm −1 under a 1.5 kOe dc field, among the largest for polynuclear transition metal SMMs. In addition, DFT and ab initio calculations suggested that the presence of a strong Co(II)−radical magnetic interaction effectively quenches the QTM effect and enhances the barrier height for the magnetization reversal.
“…20 The magnitude and sign of the magnetic exchange interactions can also be related to the calculated average total overlap integral (∑|Sa(3d)b(3d)|/n, Figure S12). 21 The smaller the average total overlap integral, the larger the ferromagnetic interaction (or the smaller the antiferromagnetic interaction) and vice versa. Note that for the J3 interaction, the JT axes of the Mn III ions lie perpendicular to each other, with one lying parallel to the bridging plane and the other perpendicular to the bridging plane.…”
<p>A [Mn<sub>18</sub>] wheel of
wheels is obtained from the reaction of MnBr<sub>2</sub> and LH<sub>3</sub> in
MeOH. The metallic skeleton reveals two asymmetric [Mn<sup>III</sup><sub>6</sub>Mn<sup>II</sup><sub>2</sub>]
squares connected into a wheel via two apical Mn<sup>II</sup> ions. Magnetic
susceptibility and magnetisation data reveal competing exchange interactions,
supported by computational studies revealing spin frustration. </p>
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