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. 2025 Feb 28;18(5):1089.
doi: 10.3390/ma18051089.

Roles of Water Molecules in the Structures and Magnetic Properties of Coordination Polymers with a Dicarboxylate Ligand

Affiliations

Roles of Water Molecules in the Structures and Magnetic Properties of Coordination Polymers with a Dicarboxylate Ligand

Dehui Zong et al. Materials (Basel). .

Abstract

Three new coordination polymers, {[M(nbpdc)(DMF)(H2O)2]·H2O} (M = Co and Ni) and [Zn(nbpdc)(DMF)(H2O)], were synthesized from 2-nitrobiphenyl-4,4'-dicarboxylate (nbpdc2-). The isomorphous Co(II) and Ni(II) compounds exhibited a two-dimensional coordination network in which the chains with single-water bridges and the chains with single-nbpdc2- bridges intersected each other by sharing the metal ions. The coordination networks were connected with uncoordinated water molecules through hydrogen bonds. The rarely identified single-water-bridged coordination chain was reinforced by water-based intrachain hydrogen bonds. The single-water bridges mediated modest antiferromagnetic superexchange in both Co(II) and Ni(II) compounds and afforded a spin-canting structure for the Co(II) compound at low temperatures. Water molecules played a distinct structural role in the Zn(II) compound, which was a one-dimensional coordination polymer with single-nbpdc2- bridges. Instead of bridging metal ions, each water molecule was coordinated to one metal ion and hydrogen-bonded to the coordination spheres of other two metal ions, resulting to an infinite ladderlike hydrogen-bonding motif. The ladders interlinked the nbpdc-bridged chains into a three-dimensional supramolecular architecture featuring the 5-conneted {44.64} net.

Keywords: cobalt; coordination polymers; hydrogen bonds; magnetic properties; nickel; spin canting; water bridges.

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Conflict of interest statement

The authors declare no conflicts of interest.

Figures

Figure 1
Figure 1
PXRD profiles of 13 compared with those simulated from the crystal data of 1 and 2.
Figure 2
Figure 2
Crystal structure of 1. (a) A view of the coordination chain formed from Zn(II) and nbpdc2− (ellipsoidal probability: 50%). The hydrogen atoms of nbpdc2− and DMF have been omitted for clarity. (b) The hydrogen-bonded ladderlike motif. (c) A view showing the stacking of the coordination chains through hydrogen bonds. The non-oxygen atoms of DMF and the nitro groups and hydrogen atoms of nbpdc2− have been omitted for clarity. (d) A topologic representation of the 3D structure composed of coordination chains (red) and hydrogen-bonded ladders (blue).
Figure 3
Figure 3
Crystal structure of 2. (a) A view of the coordination modes of Co(II) and nbpdc2− (ellipsoidal probability: 50%). The nitro group disordered over two positions is shown in light color and the hydrogen atoms of nbpdc2− and DMF have been omitted for clarity. (b) A water-bridged chain assisted with hydrogen bonds. (c) A 2D coordination layer. The non-oxygen atoms of DMF and the nitro groups and hydrogen atoms of nbpdc2− have been omitted for clarity. (d) A view of the layer packing showing interlayer hydrogen bonding. The hydrogen atoms of nbpdc2− and DMF have been omitted for clarity.
Figure 4
Figure 4
(a) Temperature dependence of χ and χT of 2 under 1 kOe. The black and red solid lines both represent the best fit to Equation (1) in the text. (b) Isothermal magnetization of 2 at 2 K. (c) FC and ZFC susceptibility of 2 under different field. (d) χ′(T) and χ″(T) plots for 2 at frequencies 10–1000 Hz with Hdc = 0 and Hac = 3.5 Oe.
Figure 5
Figure 5
Temperature dependence of χ and χT for 3 under 1 kOe. Both solid lines represent the best fit to Equation (2) in the text.

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