Magnetochemistry (Apr 2023)

Two One-Dimensional Copper-Oxalate Frameworks with the Jahn–Teller Effect: [(CH<sub>3</sub>)<sub>3</sub>NH]<sub>2</sub>[Cu(μ-C<sub>2</sub>O<sub>4</sub>)(C<sub>2</sub>O<sub>4</sub>)]·2.5H<sub>2</sub>O (I) and [(C<sub>2</sub>H<sub>5</sub>)<sub>3</sub>NH]<sub>2</sub>[Cu(μ-C<sub>2</sub>O<sub>4</sub>)(C<sub>2</sub>O<sub>4</sub>)]·H<sub>2</sub>O (II)

  • Bin Zhang,
  • Yan Zhang,
  • Zheming Wang,
  • Yang Sun,
  • Tongling Liang,
  • Mei Liu,
  • Daoben Zhu

DOI
https://doi.org/10.3390/magnetochemistry9050120
Journal volume & issue
Vol. 9, no. 5
p. 120

Abstract

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Two one-dimensional oxalate-bridged Cu(II) ammonium salts, [(CH3)3NH]2[Cu(μ-C2O4)(C2O4)]·2.5H2O (I) and [(C2H5)3NH]2[Cu(μ-C2O4)(C2O4)]·H2O (II) were obtained and characterized. They were composed of ammonium: (CH3)3NH+ in (I), (C2H5)3NH+ in (II), [Cu(μ-C2O4)(C2O4)2−]n and H2O. The Jahn–Teller-distorted Cu(II) is octahedrally coordinated by six O atoms from three oxalates and forms a one-dimensional zigzag chain. The hydrogen bonds between ammonium, the anion and H2O form a three-dimensional network. There is no hydrogen bond between the anion chains. They were insulated at 20 °C with a relative humidity of 40%. Ferromagnetic and weak-ferromagnetic behaviors were observed in I and II, separately. No long-range ordering was observed above 2 K.

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