4.6 Article

Three-Dimensional Open-Frameworks Based on LnIII Ions and Open-/Closed-Shell PTM Ligands: Synthesis, Structure, Luminescence, and Magnetic Properties

Journal

CHEMISTRY-A EUROPEAN JOURNAL
Volume 17, Issue 13, Pages 3644-3656

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/chem.201002993

Keywords

lanthanides; luminescence; magnetic properties; metal-organic frameworks; radicals

Funding

  1. EU, under contract MAGMANet [515767]
  2. Instituto de Salud Carlos III
  3. MICINN, Spain [CTQ2006-06333/BQU, CTQ2010-19501/BQU]
  4. Generalitat de Catalunya [2009SGR00516]
  5. Region Midi-Pyrenees

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A series of isostructural open-framework coordination polymers formulated as [Ln(dmf)(3)(ptmtc)] (Ln = Sm (1), Eu (2), Gd (3), Tb (4), Dy (5); PTMTC = polychlorotriphenyl-methyl tricarboxylate) and [Ln(dmf)(2)H2O(alpha H-ptmtc)] (Ln = Sm (1'), Eu (2'), Gd (3'), Tb (4'), Dy (5')) have been obtained by treating Ln(III) ions with PTMTC ligands with a radical (PTMTC3-) or a closed-shell character (alpha H-PTMTC3-). X-ray diffraction analyses reveal that these coordination polymers possess 3D architectures that combine large channels and fairly rare lattice complex T connectivity. In addition, these compounds show selective framework dynamic sorption properties. For both classes of ligands, the ability to act as an antenna in Ln sensitization processes has been investigated. No luminescence was observed for compounds 1-5, and 3' because of the PTMTC3- ligand and/or Gd-III ion characteristics. Conversely, photoluminescence measurements show that 1', 2', 4', and 5' emit dark orange, red, green, and dark cyan metal-centered luminescence. The magnetic properties of all of these compounds have been investigated. The nature of the {Ln-radical} exchange interaction in these compounds has been assessed by comparing the behavior of the radical-based coordination polymers 1-5 with those of the compounds with the diamagnetic ligand set. While antiferromagnetic {Sm-radical} interactions are found in 1, ferromagnetic {Ln-radical} interactions propagate in the 3D architectures of 3, 4, and 5 (Ln = Gd, Tb, and Dy, respectively). This procedure also provided access to information on the {Ln - Ln} exchange existing in these magnetic systems.

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