The dinuclear copper(II) complexes {[Cu2(1,3-tpbd)- (H2O)(OAc)2](ClO4)2}0.23{[Cu2(1,3-tpbd)(H2O)2(OAc)]- (ClO4)3}0.77·0.77H2O (1), [Cu2(1,3-tpbd)(H2O)2(OAc)2]- (ClO4)2·2H2O (2), and the tetranuclear copper(II) complex [Cu4(1,3-tpbd)2(H2O)2(SO4)4]·8H2O (3) {1,3-tpbd = 1,3- bis[bis(2-pyridylmethyl)amino]benzene} were synthesised and structurally characterised by X-ray diffraction. Variable temperature (2.0-290 K) magnetic susceptibility measurements on these complexes as well as on the dinuclear copper(II) complex [Cu2(1,3-tpbd)(H2O)2(ClO4)3]ClO4 (4) (whose structure was published earlier) were performed. In contrast to 2 and 3, significant ferromagnetic coupling with J = +9.3 cm-1 was observed for 4 (the Hamiltonian being defined as Hˆ = -J Sˆ 1·Sˆ 2). Density functional theory (DFT) calculations were used successfully for the interpretation of the ferromagnetic coupling observed in 4.
Foxon, S., Torres, G., Walter, O., Pedersen, J.z., Toftlund, H., Hüber, M., et al. (2004). Syntheses, structures, and magnetic properties of copper(II) complexes with 1,3-[bis(2-pyridylmethyl)amino]benzene (1,3-tpbd) as ligand. EUROPEAN JOURNAL OF INORGANIC CHEMISTRY, 2004, 335-343 [10.1002/ejic.200300426].
Syntheses, structures, and magnetic properties of copper(II) complexes with 1,3-[bis(2-pyridylmethyl)amino]benzene (1,3-tpbd) as ligand.
PEDERSEN, JENS ZACHO;
2004-01-01
Abstract
The dinuclear copper(II) complexes {[Cu2(1,3-tpbd)- (H2O)(OAc)2](ClO4)2}0.23{[Cu2(1,3-tpbd)(H2O)2(OAc)]- (ClO4)3}0.77·0.77H2O (1), [Cu2(1,3-tpbd)(H2O)2(OAc)2]- (ClO4)2·2H2O (2), and the tetranuclear copper(II) complex [Cu4(1,3-tpbd)2(H2O)2(SO4)4]·8H2O (3) {1,3-tpbd = 1,3- bis[bis(2-pyridylmethyl)amino]benzene} were synthesised and structurally characterised by X-ray diffraction. Variable temperature (2.0-290 K) magnetic susceptibility measurements on these complexes as well as on the dinuclear copper(II) complex [Cu2(1,3-tpbd)(H2O)2(ClO4)3]ClO4 (4) (whose structure was published earlier) were performed. In contrast to 2 and 3, significant ferromagnetic coupling with J = +9.3 cm-1 was observed for 4 (the Hamiltonian being defined as Hˆ = -J Sˆ 1·Sˆ 2). Density functional theory (DFT) calculations were used successfully for the interpretation of the ferromagnetic coupling observed in 4.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.