2 research outputs found

    Alkaline Ion-Modulated Solid-State Supramolecular Organization in Mixed Organic/Metallorganic Compounds Based on 1,1′-Ethylenebis(4-aminopyridinium) Cations and Bis(oxamate)cuprate(II) Anions

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    Three new coordination compounds of formula (edap)<sub>2</sub>­[Cu­(opba)]<sub>2</sub>­·4H<sub>2</sub>O (<b>1</b>), (edap)­[{Na<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>}­{Cu<sub>2</sub>(opba)<sub>2</sub>}]­·2H<sub>2</sub>O (<b>2</b>), and (edap)­[{K<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>}­{Cu<sub>2</sub>(opba)<sub>2</sub>}]­·3H<sub>2</sub>O (<b>3</b>) (edap = 1,1′-ethylenebis­(4-aminopyridinium) and opba = 1,2-phenylenebis­(oxamate)) were synthesized through the metathesis reaction involving A<sub>2</sub>[Cu­(opba)] (A = Li<sup>+</sup>, Na<sup>+</sup>, and K<sup>+</sup>) and (edap)­Cl<sub>2</sub>·2H<sub>2</sub>O. Crystal structures of <b>1</b>–<b>3</b> and edap­(IO<sub>3</sub>)<sub>2</sub>­·4H<sub>2</sub>O compound were elucidated by single crystal X-ray diffraction. Compounds <b>1</b>–<b>3</b> are built up from dinuclear copper­(II) entities, {[Cu­(opba)]<sub>2</sub>}<sup>4–</sup> with an asymmetric bis­(monatomic oxygen) bridge resulting from the parallel “out-of-plane” disposition of the planar mononuclear [Cu­(opba)]<sup>2–</sup>. They possess distinct supramolecular arrangements of varying dimensionality (<i>n</i>D with <i>n</i> = 0 (<b>1</b>), 1 (<b>2</b>), and 2 (<b>3</b>)) in the solid state depending on the nature of the coordinated alkaline ion present alongside edap<sup>2+</sup> counterions. While the {[Cu­(opba)]<sub>2</sub>}<sup>4–</sup> building blocks are well-isolated in <b>1</b>, they form either double chains or corrugated layers due to the coordination of the Na<sup>+</sup> or K<sup>+</sup> ions in <b>2</b> and <b>3</b>, respectively. Magnetic properties of <b>1</b>–<b>3</b> show a very weak antiferromagnetic coupling between the Cu<sup>II</sup> ions through a double monatomic (μ-O) bridge (−<i>J</i> = 1.63(9) (<b>1</b>), 2.29(2) (<b>2</b>), and 1.65(3) cm<sup>–1</sup> (<b>3</b>)), the Hamiltonian being defined as <i><b>H</b></i> = −(<i><b>S</b></i><sub><i><b>1</b></i></sub>·<i><b>S</b></i><sub><i><b>2</b></i></sub>) + <i>g βH</i>(<i><b>S</b></i><sub><i><b>1</b></i></sub> + <i><b>S</b></i><sub><i><b>2</b></i></sub>)

    Solvent effects on the dimensionality of oxamato-bridged manganese(II) compounds

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    <p>Two new oxamate-containing manganese(II) complexes, [{Mn(H<sub>2</sub>edpba)(H<sub>2</sub>O)<sub>2</sub>}<sub>2</sub>]<sub>n</sub> (<b>1</b>) and [Mn(H<sub>2</sub>edpba)(dmso)<sub>2</sub>]∙dmso∙CH<sub>3</sub>COCH<sub>3</sub>∙H<sub>2</sub>O (<b>2</b>) (H<sub>4</sub>edpba = <i>N,N′</i>-ethylenediphenylenebis(oxamic acid) and dmso = dimethylsulfoxide), have been synthesized and the structures of <b>1</b> and <b>2</b> were characterized by single crystal X-ray diffraction. The structure of <b>1</b> consists of neutral honeycomb networks in which each manganese(II) is six-coordinate by one H<sub>2</sub>edpba<sup>2−</sup> ligand and two carboxylate–oxygens from two other H<sub>2</sub>edpba<sup>2−</sup> ligands building the equatorial plane. Each manganese is connected to its nearest neighbor through two carboxylate(monoprotonated oxamate) bridges in an <i>anti</i>-<i>syn</i> conformation. A dmso solution of single crystals of <b>1</b> was placed under acetone atmosphere affording <b>2</b>, whereas putting <b>2</b> in equimolar water:ethanol mixture results in <b>1</b>. The molecular structure of <b>2</b> is made up of mononuclear manganese(II) units which are interlinked by weak C–H⋯π and edge-to-face π-stacking interactions leading to supramolecular chains along the crystallographic <i>b</i> axis. Magnetic measurements reveal the occurrence of an antiferromagnetic coupling between two manganese(II) ions through <i>anti-syn</i> carboxylate bridges for <b>1</b> [<i>J</i> = −1.18 cm<sup>−1</sup>, the Hamiltonian being defined as <b><i>H</i> </b>= −<i>J</i> <b><i>S</i></b><sub>1</sub><sup>.</sup><b><i>S</i></b><sub>2</sub>] and very weak intrachain ferromagnetic interactions in <b>2</b> [<i>J</i> = + 0.046 cm<sup>−1</sup>, <b><i>H</i></b> = −<i>J</i> ∑<sub>i</sub><b><i>S</i></b><sub>i</sub><sup>.</sup><b><i>S</i></b><sub>i + 1</sub>].</p
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