001     201881
005     20210129215937.0
024 7 _ |a 10.1039/c4dt00306c
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024 7 _ |a 1364-5447
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024 7 _ |a 1470-479X
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024 7 _ |a 1472-7773
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024 7 _ |a 1477-9226
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024 7 _ |a 1477-9234
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037 _ _ |a FZJ-2015-04175
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100 1 _ |a Ghisolfi, Alessio
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245 _ _ |a A comparative synthetic, magnetic and theoretical study of functional M$_{4}$Cl $_{4}$ cubane-type Co(ii) and Ni(ii) complexes
260 _ _ |a London
|c 2014
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336 7 _ |a Journal Article
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520 _ _ |a We describe the synthesis, structures, and magnetochemistry of new M4Cl4 cubane-type cobalt(II) and nickel(II) complexes with the formula [M(μ3-Cl)Cl(HL·S)]4 (1: M = Co; 2: M = Ni), where HL·S represents a pyridyl-alcohol-type ligand with a thioether functional group, introduced to allow subsequent binding to Au surfaces. Dc and ac magnetic susceptibility data of 1 and 2 were modeled with a full spin Hamiltonian implemented in the computational framework CONDON 2.0. Although both coordination clusters 1 and 2 are isostructural, with each of their transition metal ions in a pseudo-octahedral coordination environment of four Cl atoms and N,O-donor atoms of one chelating HL·S ligand, the substantially different ligand field effects of Co(II) and Ni(II) results in stark differences in their magnetism. In contrast to compound 1 which exhibits a dominant antiferromagnetic intramolecular coupling (J = −0.14 cm−1), 2 is characterised by a ferromagnetic coupling (J = +10.6 cm−1) and is considered to be a single-molecule magnet (SMM), a feature of special interest for future surface deposition studies. An analysis based on density functional theory (DFT) was performed to explore possible magnetostructural correlations in these compounds. Using a two-J model Hamiltonian, it revealed that compound 1 has four positive and two (small) negative JCoCo isotropic interactions leading to a SHS = 6 ground state. Taking into account the magnetic anisotropy, one would recover a MS = 0 ground state since D > 0 from computations. In 2, all the J constants are positive and, in this framework, the zero-field splitting energy characterising the axial anisotropy was estimated to be negative (D = −0.44 cm−1). The computational results are consistent with compound 2 being an SMM.
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700 1 _ |a Monakhov, Kirill Yu.
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700 1 _ |a Pattacini, Roberto
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700 1 _ |a Braunstein, Pierre
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700 1 _ |a López, Xavier
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700 1 _ |a de Graaf, Coen
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700 1 _ |a Speldrich, Manfred
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700 1 _ |a van Leusen, Jan
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700 1 _ |a Schilder, Helmut
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700 1 _ |a Kögerler, Paul
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773 _ _ |a 10.1039/c4dt00306c
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