Structural and magnetic properties of one-dimensional coordination polymers {trans-[Ru(C≡N-ᵗBu)₄(CN)₂]FeX₃}ₙ vs. molecular squares {cis-[Ru(C≡N-ᵗBu)₄(CN)₂]FeX₃}₂ (X = NO₃, Cl)
Inorganica Chimica Acta. Bd. 363. H. 5. Amsterdam: Elsevier 2010 S. 1013 - 1020
Erscheinungsjahr: 2010
ISBN/ISSN: 0020-1693
Publikationstyp: Zeitschriftenaufsatz
Sprache: Englisch
Doi/URN: 10.1016/j.ica.2009.12.021
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Inhaltszusammenfassung
The reaction of cis- or trans-[Ru(C (NBu)-Bu-t)(4)(CN)(2)] with Fe(III) compounds leads to the formation of molecular squares of the general formula cyc-[Ru(C N-Bu-t)(4)(CN)(2)FeX3](2) or one-dimensional coordination polymers [Ru(C N-Bu-t)(4)(CN)(2)FeX3](n), respectively. Temperature dependent susceptibility measurements indicate that the magnetic properties of the coordination compounds are determined by their molecular structure. Of particular importance is the local symmetry at the iron(...The reaction of cis- or trans-[Ru(C (NBu)-Bu-t)(4)(CN)(2)] with Fe(III) compounds leads to the formation of molecular squares of the general formula cyc-[Ru(C N-Bu-t)(4)(CN)(2)FeX3](2) or one-dimensional coordination polymers [Ru(C N-Bu-t)(4)(CN)(2)FeX3](n), respectively. Temperature dependent susceptibility measurements indicate that the magnetic properties of the coordination compounds are determined by their molecular structure. Of particular importance is the local symmetry at the iron( III) center which is related to the coordinating anion. The magnetic properties are best described in terms of weak antiferromagnetic interactions between the iron centers for the molecular squares as well as the coordination polymer with X = NO3 and as weak ferromagnetic interactions in case of the linear coordination polymer with X = Cl. For all compounds zero field splitting at low temperatures has to be taken into account. (C) 2009 Elsevier B.V. All rights reserved. » weiterlesen» einklappen