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Conducting Anilate-Based Mixed-Valence Fe(II)Fe(III) Coordination Polymer: Small-Polaron Hopping Model for Oxalate-Type Fe(II)Fe(III) 2D Networks

  • Suchithra Ashoka Sahadevan
    Suchithra Ashoka Sahadevan
    Laboratoire MOLTECH-Anjou UMR 6200, UFR Sciences, CNRS, Université d’Angers, Bât. K, 2 Bd. Lavoisier, 49045 Angers, France
    Dipartimento di Scienze Chimiche e Geologiche, Università degli Studi di Cagliari, I-09042 Monserrato (Cagliari), Italy
  • Alexandre Abhervé
    Alexandre Abhervé
    Laboratoire MOLTECH-Anjou UMR 6200, UFR Sciences, CNRS, Université d’Angers, Bât. K, 2 Bd. Lavoisier, 49045 Angers, France
  • Noemi Monni
    Noemi Monni
    Dipartimento di Scienze Chimiche e Geologiche, Università degli Studi di Cagliari, I-09042 Monserrato (Cagliari), Italy
    More by Noemi Monni
  • Cristina Sáenz de Pipaón
    Cristina Sáenz de Pipaón
    Institute of Chemical Research of Catalonia, The Barcelona Institute of Science and Technology (BIST), Avenida Països Catalans 16, 43007 Tarragona, Spain
  • José Ramón Galán-Mascarós
    José Ramón Galán-Mascarós
    Institute of Chemical Research of Catalonia, The Barcelona Institute of Science and Technology (BIST), Avenida Països Catalans 16, 43007 Tarragona, Spain
    ICREA, Passeig Lluís Companys 23, 08010 Barcelona, Spain
  • João C. Waerenborgh
    João C. Waerenborgh
    Centro de Ciências e Tecnologias Nucleares, Instituto Superior Técnico, Universidade de Lisboa, 2695-066 Bobadela LRS, Portugal
  • Bruno J. C. Vieira
    Bruno J. C. Vieira
    Centro de Ciências e Tecnologias Nucleares, Instituto Superior Técnico, Universidade de Lisboa, 2695-066 Bobadela LRS, Portugal
  • Pascale Auban-Senzier
    Pascale Auban-Senzier
    Laboratoire de Physique des Solides, UMR 8502, Bât. 510, CNRS-Université Paris-Sud, 91405 Orsay, France
  • Sébastien Pillet
    Sébastien Pillet
    Université de Lorraine, CNRS, CRM2, F-54000 Nancy, France
  • El-Eulmi Bendeif
    El-Eulmi Bendeif
    Université de Lorraine, CNRS, CRM2, F-54000 Nancy, France
  • Pere Alemany*
    Pere Alemany
    Departament de Ciència de Materials i Química Física and Institut de Química Teòrica i Computacional (IQTCUB), Universitat de Barcelona, Martí i Franquès 1, 08028 Barcelona, Spain
    *[email protected]
    More by Pere Alemany
  • Enric Canadell*
    Enric Canadell
    Institut de Ciència de Materials de Barcelona (CSIC), Campus de la UAB, E-08193 Bellaterra, Spain
    *[email protected]
  • Maria Laura Mercuri*
    Maria Laura Mercuri
    Dipartimento di Scienze Chimiche e Geologiche, Università degli Studi di Cagliari, I-09042 Monserrato (Cagliari), Italy
    *[email protected]
  • , and 
  • Narcis Avarvari*
    Narcis Avarvari
    Laboratoire MOLTECH-Anjou UMR 6200, UFR Sciences, CNRS, Université d’Angers, Bât. K, 2 Bd. Lavoisier, 49045 Angers, France
    *[email protected]
Cite this: J. Am. Chem. Soc. 2018, 140, 39, 12611–12621
Publication Date (Web):September 10, 2018
https://doi.org/10.1021/jacs.8b08032
Copyright © 2018 American Chemical Society
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Supporting Info (3)»

Abstract

Abstract Image

The mixed-valence FeIIFeIII 2D coordination polymer formulated as [TAG][FeIIFeIII(ClCNAn)3]·(solvate) 1 (TAG = tris(amino)-guanidinium, ClCNAn2– = chlorocyanoanilate dianionic ligand) crystallized in the polar trigonal space group P3. In the solid-state structure, determined both at 150 and at 10 K, anionic 2D honeycomb layers [FeIIFeIII(ClCNAn)3] establish in the ab plane, with an intralayer metal–metal distance of 7.860 Å, alternating with cationic layers of TAG. The similar Fe–O distances suggest electron delocalization and an average oxidation state of +2.5 for each Fe center. The cation imposes its C3 symmetry to the structure and engages in intermolecular N–H···Cl hydrogen bonding with the ligand. Magnetic susceptibility characterization indicates magnetic ordering below 4 K and the presence of a hysteresis loop at 2 K with a coercive field of 60 Oe. Mössbauer measurements are in agreement with the existence of Fe(+2.5) ions at RT and statistic charge localization at 10 K. The compound shows semiconducting behavior with the in-plane conductivity of 2 × 10–3 S/cm, 3 orders of magnitude higher than the perpendicular one. A small-polaron hopping model has been applied to a series of oxalate-type FeIIFeIII 2D coordination polymers, providing a clear explanation on the much higher conductivity of the anilate-based systems than the oxalate ones.

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