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Orbital‐dependent magnetic properties of molecular cluster containing high‐spin Co(II) ions
Author(s) -
Wang Fan,
Zhao Fei,
Wang BingWu,
Wang MingWei,
Zhang YuanZhu,
Wang Wei,
Gao Song,
Chen ZhiDa
Publication year - 2009
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.22137
Subject(s) - chemistry , hamiltonian (control theory) , cluster (spacecraft) , crystallography , exchange interaction , angular momentum , metal , magnetic susceptibility , stereochemistry , ferromagnetism , condensed matter physics , physics , quantum mechanics , mathematical optimization , mathematics , organic chemistry , computer science , programming language
To shed light on magnetic properties of the magnetic exchange molecular cluster containing the constituent metal ion with unquenched orbital angular momentum, as representative examples two octahedrally coordinated high‐spin Co(II)‐cluster complexes were synthesized and characterized: complex ( 1 ) [Co 3 (Hbzp) 6 ][ClO 4 ] 2 · 2CH 3 OH·H 2 O (bzp = 2‐benzoylpyridine) with a linear core Co(III)‐Co(II)‐Co(III) and complex ( 2 ) [Co 4 L(N 3 ) 4 (CH 3 CN) 4 ](ClO 4 ) 4 · 2H 2 O (L = Macrocyclic schiff base of tetra‐2,6‐pyridinedicarboxaldehyde‐tetra‐ethane‐1,2‐diamine) comprised by two nearly independent Co(II)‐dimers. Following Lines' isotropic exchange approximation the magnetic interaction effective Hamiltonian was introduced, which includes the exchange interactions, the spin‐orbit coupling, the low‐symmetry crystal field, and the intercluster exchange interaction. On the basis of the irreducible tensor operator approach to solve Hamiltonian we have coded the software, BJMAG package, and performed the best‐fit procedure for experimentally temperature variable magnetic susceptibilities for the complexes ( 1 ) and ( 2 ). The best‐fit parameters were obtained as follows: λ = −126 cm −1 , Δ = 432 cm −1 , κ = 0.96, mJ ′ = 2.7 cm −1 for the complex ( 1 ) and λ = −165 cm −1 , Δ = 960 cm −1 , κ = 0.95, J ′ = 9 cm −1 , mJ ′ = −0.1 cm −1 for the complex ( 2 ). To further elucidate the individual role of each interaction in the employed model, the effects of the key factors governing the magnetic properties on temperature variable magnetic susceptibilities were examined in detail. The significance of the intercluster exchange interactions at low temperatures was briefly discussed and a self‐consistent molecular field to calculate the thermally average spin of the nearest neighbor in the intercluster interaction was proposed. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2009