Homoleptic Organocobalt(III) Compounds with Intermediate Spin

Homoleptic organocobalt­(III) compounds with formula [NBu4]­[CoIII(C6X5)4] [X = F (3), Cl (4)] were obtained in reasonable yields by chemical oxidation of the corresponding divalent species [NBu4]2­[CoII(C6X5)4] [X = F (1), Cl (2)]. The [CoIII(C6X5)4]−/[CoII(C6X5)4]2– couples are electrochemically r...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Inorganic chemistry 2014-12, Vol.53 (23), p.12384-12395
Hauptverfasser: García-Monforte, M. Angeles, Ara, Irene, Martín, Antonio, Menjón, Babil, Tomás, Milagros, Alonso, Pablo J, Arauzo, Ana B, Martínez, Jesús I, Rillo, Conrado
Format: Artikel
Sprache:eng
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:Homoleptic organocobalt­(III) compounds with formula [NBu4]­[CoIII(C6X5)4] [X = F (3), Cl (4)] were obtained in reasonable yields by chemical oxidation of the corresponding divalent species [NBu4]2­[CoII(C6X5)4] [X = F (1), Cl (2)]. The [CoIII(C6X5)4]−/[CoII(C6X5)4]2– couples are electrochemically related by quasi-reversible, one-electron exchange processes at moderate potential: E 1/2 = −0.29 (X = F) and −0.36 V (X = Cl) versus saturated calomel electrode. The [CoIII(C6X5)4]− anions in salts 3 and 4 show an unusual square-planar geometry as established by single-crystal X-ray diffraction methods. According to their stereochemistry, these CoIII derivatives (d6) are paramagnetic non-Kramers systems with a large zero-field splitting contribution and no observable electron paramagnetic resonance (EPR) spectrum. The thermal dependence of their magnetic susceptibilities can be explained in terms of a spin-Hamiltonian formalism with S = 1 ground state (intermediate spin) and substantial spin–orbit contribution. The magnetic properties of the square-planar d7 parent species [NBu4]2­[CoII(C6X5)4] were also thoroughly studied both at microscopic (EPR) and macroscopic levels (alternating current and direct current magnetization measurements). They behave as S = 1/2 (low spin) systems with mainly (d z 2 )1 electron configuration and a certain degree of s-orbital admixture that has been quantified. The electronic structures of all four open-shell [Co­(C6X5)4] q− compounds (q = 1, 2) accounting for their respective magnetic properties are based on a common orbital energy-level diagram.
ISSN:0020-1669
1520-510X
DOI:10.1021/ic501719y