4.7 Article

Field-induced single molecule magnet behavior of a dinuclear cobalt(II) complex: a combined experimental and theoretical study

Journal

DALTON TRANSACTIONS
Volume 49, Issue 46, Pages 16778-16790

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d0dt02158j

Keywords

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Funding

  1. UGC, India
  2. Spanish MINECO [CTQ2017-87201-P AEI/FEDER, Prometeo/2019/076]

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Two dinuclear cobalt(II) complexes, [(dmso)(CoL1)-L-II(mu-(m-NO2)C6H4COO)Co-II(NCS)] (1) and [(dmso)(CoL2)-L-II(mu-(m-NO2)C6H4COO)Co-II(NCS)] (2) [dmso = dimethylsulfoxide, H2L1 = (2,2-dimethyl-1,3-propanediyl)bis(iminomethylene)bis(6-methoxyphenol) and H2L2 = (2,2-dimethyl-1,3-propanediyl)bis(iminomethylene)bis(6-ethoxyphenol)] have been synthesized and structurally characterized by single-crystal X-ray diffraction, magnetic-susceptibility measurements and various spectroscopic techniques. Each complex contains a cobalt(II) center with a slightly distorted octahedral geometry and a second cobalt(II) center with a distorted trigonal prismatic one. To obtain insight into the physical nature of weak non-covalent interactions, we have extensively used the Bader's quantum theory of atoms-in-molecules (QTAIM). In addition, the non-covalent interaction reduced density gradient (NCI-RDG) methods established the presence of such non-covalent intermolecular interactions. Variable temperature magnetic susceptibility measurements show that both cobalt centers in each complex are in the high spin state (S = 3/2) and both complexes show weak ferromagnetic couplings through the double phenoxido bridges (J = 3.36(3) cm(-1) in 1 and 4.56(2) cm(-1) in 2). The magnetic properties of both complexes can be fitted to a Co(ii) dimer model including similar orbital reduction factors (alpha = -0.94(1) for 1 and -0.85(1) for 2) although different zero field splitting parameters D(1) = 11.0(4) cm(-1) and D(2) = 19.5(4) cm(-1) in 1 and D(1) = 8.2(4) cm(-1) and D(2) = -1.3(4) cm(-1) in 2. AC magnetic measurements reveal that the CoII2 unit in complex 2 exhibits field-induced slow relaxation of the magnetization at low temperatures and high frequencies.

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