2011
DOI: 10.1139/v11-083
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Copper(II) complexes of open-chain thioether ligands terminated by salicylaldimine functionality*This article has a companion paper in this issue (doi: 10.1139/v11-081).

Abstract: From 1,11-bis(salicylaldimine)-3,6,9-trithiaundecane (H 2 L1), 1,11-bis(salicylaldimine)-6-oxa-3,9-dithiaundecane (H 2 L2), and 1,8-bis(salicylaldimine)-3,6-dithiaundecane (H 2 L3), syntheses for [Cu(L1)] 2 (I), Cu(L2)·CH 3 OH (II), Cu(L3) (III), [Cu(HL3)][CH 3 COO] (IV), [Cu(HL1-sal)]Cl 2 (V), Cu 4 (L1) 2 Br 4 (H 2 O) 2 ·2H 2 O (VI) and Cu 2 (L2)Br 2 ·xH 2 O (VII) are described. Single crystal X-ray structural studies for I, III and VII are reported. Variable temperature magnetic susceptibility studies of I, … Show more

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“…A search through the literature has revealed CuCu to have the largest ferromagnetic coupling for a Schiff base-derived normalC normalu 2 normalI normalI dimer to the best of our knowledge. The ferromagnetic exchange observed is unexpected based on previous magneto–structural correlations of O-bridged Cu II dimers, which consider only the Cu–O–Cu angles. The Cu1–O–Cu2 angles in CuCu are 106.01(10)° and 105.22(10)° and would be expected to promote strong antiferromagnetic interactions based on this model, as shown by similar Schiff base-derived Cu II dimers. Thus, as discussed by Ruiz and coworkers, other structural factors in CuCu including complex asymmetry, metal ion geometry, O–Cu–O–Cu torsion angles, the out-of-plane shift of the phenolato units, and the seven-coordinate Cu II ion should be considered. This will require detailed theoretical calculations, which are beyond the scope of this paper. = prefix− 2 i < j J i j true s i 0em ̂ · true s j 0em ̂ …”
Section: Resultsmentioning
confidence: 53%
“…A search through the literature has revealed CuCu to have the largest ferromagnetic coupling for a Schiff base-derived normalC normalu 2 normalI normalI dimer to the best of our knowledge. The ferromagnetic exchange observed is unexpected based on previous magneto–structural correlations of O-bridged Cu II dimers, which consider only the Cu–O–Cu angles. The Cu1–O–Cu2 angles in CuCu are 106.01(10)° and 105.22(10)° and would be expected to promote strong antiferromagnetic interactions based on this model, as shown by similar Schiff base-derived Cu II dimers. Thus, as discussed by Ruiz and coworkers, other structural factors in CuCu including complex asymmetry, metal ion geometry, O–Cu–O–Cu torsion angles, the out-of-plane shift of the phenolato units, and the seven-coordinate Cu II ion should be considered. This will require detailed theoretical calculations, which are beyond the scope of this paper. = prefix− 2 i < j J i j true s i 0em ̂ · true s j 0em ̂ …”
Section: Resultsmentioning
confidence: 53%