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3D isomorphous lanthanide coordination polymers displaying magnetic refrigeration, slow magnetic relaxation and tunable proton conduction
61
Citations
120
References
2018
Year
Four new isostructural lanthanide-based three-dimensional (3D) coordination polymers (CPs), {[Ln<sub>4</sub>(OH)<sub>4</sub>(L)<sub>2</sub>(H<sub>2</sub>O)<sub>8</sub>]·4.6H<sub>2</sub>O·1.4CH<sub>3</sub>CN}<sub>n</sub> (Ln<sup>3+</sup> = Gd<sup>3+</sup> (1), Dy<sup>3+</sup> (2), Ho<sup>3+</sup> (3) and Er<sup>3+</sup> (4)), have been constructed using a sulfonate-carboxylate-based ligand (Na<sub>2</sub>H<sub>2</sub>L = disodium-2,2'-disulfonate-4,4'-oxydibenzoic acid) and the corresponding lanthanide metal(iii) nitrates. All the CPs 1-4 contain [Ln<sub>4</sub>(μ<sub>3</sub>-OH)<sub>4</sub>]<sup>8+</sup> cubane-like cores interconnected through L<sup>4-</sup> ligands to give rise to 3D coordination frameworks with 1D hydrophilic channels along the crystallographic c direction. From the topological perspective, the underlying 3D nets of the CPs can be classified as a 3,6,6-c net with an undocumented topology. Magnetic studies display that CP 1 exhibits a magnetocaloric effect with a significant magnetic entropy change (-ΔS<sub>m</sub>) = 34.6 J kg<sup>-1</sup> K<sup>-1</sup> for ΔH = 7 T at 3 K. CP 2 shows field-induced slow magnetic relaxation properties with energy barrier (U<sub>eff</sub>/k<sub>B</sub>) = 30.40 K and relaxation time (τ<sub>0</sub>) = 2.47 × 10<sup>-7</sup> s. Theoretical calculations have been performed to corroborate the magnetic exchange coupling constant value for CP 1 and to obtain a deeper understanding of the field-induced slow magnetic relaxation behavior of CP 2. Impedance analyses display high values of proton conductivity which reach 2.02 × 10<sup>-6</sup>, 2.96 × 10<sup>-6</sup>, 4.56 × 10<sup>-3</sup> and 6.59 × 10<sup>-3</sup> S cm<sup>-1</sup> for CPs 1-4, respectively at high temperature (>75 °C) and 95% relative humidity (RH) in the order CP 1 < CP 2 < CP 3 < CP 4. Notably, the proton conductivities for CPs 3 and 4 are a few orders of magnitude higher than those of CPs 1 and 2 (10<sup>-3</sup> S cm<sup>-1</sup>vs. 10<sup>-6</sup> S cm<sup>-1</sup>), and the conductivity increases periodically following the decreasing order of ionic radius (Gd<sup>3+</sup> > Dy<sup>3+</sup> > Ho<sup>3+</sup> > Er<sup>3+</sup>). This demonstrates the effective employment of the lanthanide contraction strategy to tune proton conductivity while preserving proton-conducting pathways.
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