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High‐Temperature Experimental and Theoretical Study of Magnetic Interactions in Diamond and Pseudo‐Diamond Frameworks Built up from Hexanuclear Tantalum Clusters
Author(s) -
Perić Berislav,
Cordier Stéphane,
Cuny Jérôme,
Gautier Régis,
Guizouarn Thierry,
Planinić Pavica
Publication year - 2011
Publication title -
chemistry – a european journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.687
H-Index - 242
eISSN - 1521-3765
pISSN - 0947-6539
DOI - 10.1002/chem.201002332
Subject(s) - tantalum , crystallography , diamond , paramagnetism , chemistry , cluster (spacecraft) , octahedron , magnetic susceptibility , tetragonal crystal system , bromine , condensed matter physics , crystal structure , physics , organic chemistry , computer science , programming language
Magnetic interactions in solid‐state tantalum cluster compounds have been evidenced by using magnetic susceptibility measurements and corroborated by broken‐symmetry DFT calculations. The three selected compounds are based on [Ta 6 X 12 (H 2 O) 6 ] 3+ (X=Cl or/and Br) units with edge‐bridged Ta 6 octahedral clusters. Although two of them crystallise in the tetragonal space group I 4 1 / a , all compounds exhibit a similar arrangement of paramagnetic clusters related to the diamond structural framework ( Fd $\bar 3$ m space group). Magnetic parameters were fitted by using the [5,4] Padé approximant of high‐temperature series expansion of susceptibility for the Heisenberg model ( S =1/2) in the diamond framework, assuming only nearest‐neighbouring interactions. Such a model appropriately describes magnetic‐susceptibility measurements at temperatures T >0.7| J |/ k . The magnetic interaction parameter J between two [Ta 6 Cl 12 (H 2 O) 6 ] 3+ clusters is estimated to be −64.28(7) cm −1 ; it has been enhanced by replacing several chlorine inner ligands with bromine ones ( J =−123(3) cm −1 for two [Ta 6 Br 7.7(1) Cl 4.3(1) (H 2 O) 6 ] 3+ clusters) and is strongest between two bromine [Ta 6 Br 12 (H 2 O) 6 ] 3+ clusters with a value of −155(1) cm −1 . Broken‐symmetry DFT calculations within spin–dimer analysis confirmed this trend. Those interactions can be explained on the basis of the overlap between singly occupied a 2u orbitals localised on neighbouring clusters.

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