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Mono- and Binuclear Copper(II) and Nickel(II) Complexes with the 3,6-Bis(picolylamino)-1,2,4,5-Tetrazine Ligand
Four new compounds of formulas [Cu(hfac)(2)(L)] (1), [Ni(hfac)(2)(L)] (2), [{Cu(hfac)(2)}(2)(µ-L)]·2CH(3)OH (3) and [{Ni(hfac)(2)}(2)(µ-L)]·2CH(3)CN (4) [Hhfac = hexafluoroacetylacetone and L = 3,6-bis(picolylamino)-1,2,4,5-tetrazine] have been prepared and their structures determined by X-ray diffr...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8067877/ https://www.ncbi.nlm.nih.gov/pubmed/33917122 http://dx.doi.org/10.3390/molecules26082122 |
Sumario: | Four new compounds of formulas [Cu(hfac)(2)(L)] (1), [Ni(hfac)(2)(L)] (2), [{Cu(hfac)(2)}(2)(µ-L)]·2CH(3)OH (3) and [{Ni(hfac)(2)}(2)(µ-L)]·2CH(3)CN (4) [Hhfac = hexafluoroacetylacetone and L = 3,6-bis(picolylamino)-1,2,4,5-tetrazine] have been prepared and their structures determined by X-ray diffraction on single crystals. Compounds 1 and 2 are isostructural mononuclear complexes where the metal ions [copper(II) (1) and nickel(II) (2)] are six-coordinated in distorted octahedral MN(2)O(4) surroundings which are built by two bidentate hfac ligands plus another bidentate L molecule. This last ligand coordinates to the metal ions through the nitrogen atoms of the picolylamine fragment. Compounds 3 and 4 are centrosymmetric homodinuclear compounds where two bidentate hfac units are the bidentate capping ligands at each metal center and a bis-bidentate L molecule acts as a bridge. The values of the intramolecular metal···metal separation are 7.97 (3) and 7.82 Å (4). Static (dc) magnetic susceptibility measurements were carried out for polycrystalline samples 1–4 in the temperature range 1.9–300 K. Curie law behaviors were observed for 1 and 2, the downturn of χ(M)T in the low temperature region for 2 being due to the zero-field splitting of the nickel(II) ion. Very weak [J = −0.247(2) cm(−1)] and relatively weak intramolecular antiferromagnetic interactions [J = −4.86(2) cm(−1)] occurred in 3 and 4, respectively (the spin Hamiltonian being defined as H = −JS(1)·S(2)). Simple symmetry considerations about the overlap between the magnetic orbitals across the extended bis-bidentate L bridge in 3 and 4 account for their magnetic properties. |
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