Role of steric crowding of ligands in the formation of hydroxido bridged di- and trinuclear copper(II) complexes: Structures and magnetic properties

Bhowmik, Pallab ; Jana, Subrata ; Mahapatra, Prithwish ; Giri, Sanjib ; Chattopadhyay, Shouvik ; Ghosh, Ashutosh (2018) Role of steric crowding of ligands in the formation of hydroxido bridged di- and trinuclear copper(II) complexes: Structures and magnetic properties Polyhedron, 145 . pp. 43-52. ISSN 0277-5387

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Official URL: http://doi.org/10.1016/j.poly.2018.01.026

Related URL: http://dx.doi.org/10.1016/j.poly.2018.01.026

Abstract

Two new trinuclear copper(II) complexes, [(CuL1)3(μ3-OH)](ClO4)2 (1) and [(CuL2)3(μ3-OH)](ClO4)2·5H2O (2), and one new dinuclear Cu(II) complex, [(CuL3)2(μ2-OH)(CH3OH)]ClO4 (3), have been synthesized using three tridentate NNO donor Schiff bases, HL1, HL2 and HL3 (HL1 = 1-((2-aminoethylimino)methyl)naphthalen-2-ol, HL2 = 1-((2-(methylamino)ethylimino)methyl)naphthalen-2-ol and HL3 = 1-((2-(dimethylamino)ethylimino)methyl)naphthalen-2-ol), respectively and structurally characterized by single-crystal X-ray diffraction. Complexes 1 and 2 consist of trinuclear [(CuL)3(μ3-OH)]2+ units, whereas 3 contains dinuclear [(CuL)2(μ2-OH)]+ unit along, with perchlorate anions which are needed to balance the charge. In each of the complexes, all the copper atoms are five-coordinated with a distorted square-pyramidal geometry, except for complex 1 in which one of the Cu(II) ions of the trinuclear unit is six-coordinate, being weakly coordinated to one of the perchlorate anions to form an elongated distorted octahedron. The equatorial plane consists of the bridging oxygen of the central OH− group together with three atoms (NNO) from the Schiff base. The phenoxido oxygen atom of the Schiff base coordinates to the axial position of the Cu(II) ion of another subunit to form the cyclic trimer in 1 and 2 and dimer in 3. Magnetic measurements of complexes 1–3 in the 2–300 K temperature range indicate antiferromagnetic coupling in the complexes with J = −8.85, −4.86 and −50.60 cm−1 for 1–3 respectively. Density Functional Theory has also been performed in order to estimate the exchange coupling constants in these three complexes. The theoretically calculated J values are in good agreement with the experimental values.

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