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Electronic Structures of the Electron Transfer Series [M(bpy)<sub>3</sub>]<i><sup>n</sup></i>, [M(tpy)<sub>2</sub>]<i><sup>n</sup></i>, and [Fe(<sup>t</sup>bpy)<sub>3</sub>]<i><sup>n</sup></i> (M = Fe, Ru; <i>n</i> = 3+, 2+, 1+, 0, 1–): A Mössbauer Spectroscopic and DFT Study
100
Citations
86
References
2012
Year
Bpy 0EngineeringChemistryDft StudyElectronic StructureInorganic CompoundQuantum MaterialsMossbauer SpectroscopyMaterials ScienceInorganic ChemistryPhysicsT BpyDft CalculationsQuantum ChemistryInorganic SynthesisNatural SciencesCoordination ComplexCondensed Matter PhysicsMössbauer SpectroscopicElectronic StructuresMolecular Complex
Abstract The five‐membered electron‐transfer series [M(bpy) 3 ] n and [M(tpy) 2 ] n (M = Fe, Ru; bpy = 2,2′‐bipyridine, tpy = 2,2′:6′,2″‐terpyridine) and [Fe( t bpy) 3 ] n ( t bpy = 4,4′‐di‐ tert ‐butyl‐2,2′‐bipyridine; n = 3+, 2+, 1+, 0, 1–) have been investigated and the electronic structure of the so called “low‐valent” complexes ( n = 1+, 0, 1–) have been established by a combination of electro‐ and magnetochemistry, electron paramagnetic resonance (EPR) and Mössbauer spectroscopy, X‐ray crystallography, and DFT calculations. These complexes are accessed by reduction of the d 6 S = 0 dicationic starting materials [M(bpy) 3 ] 2+ and [M(tpy) 2 ] 2+ (M = Fe, Ru) and [Fe( t bpy) 3 ] 2+ . The monocations [M(bpy · )(bpy 0 ) 2 ] 1+ ( S = 1/2) and [M(tpy · )(tpy 0 )] 1+ ( S = 1/2) (M = Fe II , Ru II ) also contain a low‐spin (t 2g ) 6 divalent metal center, plus a single radical monoanion (bpy · ) 1– or (tpy · ) 1– , and two or one neutral (bpy 0 ) or (tpy 0 ) ligands, respectively. The unpaired electron resides in a ligand π* orbital. The neutral complexes [Fe II (bpy · ) 2 (bpy 0 )] 0 and [Ru II (tpy · ) 2 ] 0 were found, by DFT calculations, to possess an S = 1 ground state that is attained by weak intramolecular ferromagnetic coupling between two ligand radical anions and a singlet excited state ( S = 0). In contrast, the neutral species [Ru II (bpy · ) 2 (bpy 0 )] 0 possesses an S = 0 ground state. The metal centers of these neutral complexes retain a low‐spin (t 2g ) 6 configuration. Remarkably, the corresponding neutral complex [Fe II (tpy · ) 2 ] 0 contains high‐spin Fe II ( S Fe = 2). Strong intramolecular antiferromagnetic metal–radical coupling yields an experimentally observed S = 1 ground state. The monoanions [M II (bpy · ) 3 ] 1– (M = Fe, Ru) are composed of a low‐spin metal ion [Fe, Ru; (t 2g ) 6 ; S M = 0] and three (bpy · ) 1– radical anions.
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