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Structures and Magnetic Properties of an Antiferromagnetically Coupled Polymeric Copper(II) Complex and Ferromagnetically Coupled Hexanuclear Nickel(II) Clusters

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https://figshare.com/articles/dataset/Structures_and_Magnetic_Properties_of_an_Antiferromagnetically_Coupled_Polymeric_Copper_II_Complex_and_Ferromagnetically_Coupled_Hexanuclear_Nickel_II_Clusters/2544550
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Reactions between 2,6-diformyl-4-methylphenol (DFMF) and tris­(hydroxymethyl) aminomethane (THMAM = H3L2) in the presence of copper­(II) salts, CuX2 (X = CH3CO2–, BF4–, ClO4–, Cl–, NO3–) and Ni­(CH3CO2)2 or Ni­(ClO4)2/NaC6H5CO2, sodium azide (NaN3), and triethylamine (TEA), in one pot self-assemble giving a coordination polymer consisting of repeating pentanuclear copper­(II) clusters {[Cu2(H5L2–)­(μ-N3)]2[Cu­(N3)4]·2CH3OH}n (1) and hexanuclear Ni­(II) complexes [Ni6(H3L1–)2(HL22–)2(μ-N3)4(CH3CO2)2]·6C3H7NO·C2H5OH (2) and [Ni6(H3L1–)2(HL22–)2(μ-N3)4(C6H5CO2)2]·3C3H7NO·3H2O·CH3OH (3). In 1, H5L2– and in 2 and 3 H3L1– and HL22– represent doubly deprotonated, singly deprotonated, and doubly deprotonated Schiff-base ligands H7L and H4L1 and a tripodal ligand H3L2, respectively. 1 has a novel double-stranded ladder-like structure in which [Cu­(N3)4]2– anions link single chains comprised of dinuclear cationic subunits [Cu2(H5L2–)­(μ-N3)]+, forming a 3D structure of interconnected ladders through H bonding. Nickel­(II) clusters 2 and 3 have very similar neutral hexanuclear cores in which six nickel­(II) ions are bonded to two H4L1, two H3L2, four μ-azido, and two μ-CH3CO2–/μ-C6H5CO2– ligands. In each structure two terminal dinickel (Ni2) units are connected to the central dinickel unit through four doubly bridging end-on (EO) μ-azido and four triply bridging μ3-methoxy bridges organizing into hexanuclear units. In each terminal dinuclear unit two nickel centers are bridged through one μ-phenolate oxygen from H3L1–, one μ3-methoxy oxygen from HL22–, and one μ-CH3CO2– (2)/μ-C6H5CO2– (3) ion. Bulk magnetization measurements on 1 show moderately strong antiferromagnetic coupling within the [Cu2] building block (J1 = −113.5 cm–1). Bulk magnetization measurements on 2 and 3 demonstrate that the magnetic interactions are completely dominated by ferromagnetic coupling occurring between Ni­(II) ions for all bridges with coupling constants (J1, J2, and J3) ranging from 2.10 to 14.56 cm–1 (in the Ĥ = –J1(Ŝ1Ŝ2) – J1(Ŝ2Ŝ3) – J2(Ŝ3Ŝ4) – J1(Ŝ4Ŝ5) – J1(Ŝ5Ŝ6) – J2(Ŝ1Ŝ6) – J3(Ŝ2Ŝ6) – J3(Ŝ2Ŝ5) – J3(Ŝ3Ŝ5) convention).
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