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High electrical conductivity and high porosity in a Guest@MOF material: evidence of TCNQ ordering within Cu(3)BTC(2) micropores

The host–guest system TCNQ@Cu(3)BTC(2) (TCNQ = 7,7,8,8-tetracyanoquinodimethane, BTC = 1,3,5-benzenetricarboxylate) is a striking example of how semiconductivity can be introduced by guest incorporation in an otherwise insulating parent material. Exhibiting both microporosity and semiconducting beha...

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Detalles Bibliográficos
Autores principales: Schneider, Christian, Ukaj, Dardan, Koerver, Raimund, Talin, A. Alec, Kieslich, Gregor, Pujari, Sidharam P., Zuilhof, Han, Janek, Jürgen, Allendorf, Mark D., Fischer, Roland A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6237122/
https://www.ncbi.nlm.nih.gov/pubmed/30542544
http://dx.doi.org/10.1039/c8sc02471e
Descripción
Sumario:The host–guest system TCNQ@Cu(3)BTC(2) (TCNQ = 7,7,8,8-tetracyanoquinodimethane, BTC = 1,3,5-benzenetricarboxylate) is a striking example of how semiconductivity can be introduced by guest incorporation in an otherwise insulating parent material. Exhibiting both microporosity and semiconducting behavior such materials offer exciting opportunities as next-generation sensor materials. Here, we apply a solvent-free vapor phase loading under rigorous exclusion of moisture, obtaining a series of the general formula xTCNQ@Cu(3)BTC(2) (0 ≤ x ≤ 1.0). By using powder X-ray diffraction, infrared and X-ray absorption spectroscopy together with scanning electron microscopy and porosimetry, we provide the first structural evidence for a systematic preferential arrangement of TCNQ along the (111) lattice plane and the bridging coordination motif to two neighbouring Cu-paddlewheels, as was predicted by theory. For 1.0TCNQ@Cu(3)BTC(2) we find a specific electrical conductivity of up to 1.5 × 10(–4) S cm(–1) whilst maintaining a high BET surface area of 573.7 m(2) g(–1). These values are unmatched by MOFs with equally high electrical conductivity, making the material attractive for applications such as super capacitors and chemiresistors. Our results represent the crucial missing link needed to firmly establish the structure–property relationship revealed in TCNQ@Cu(3)BTC(2), thereby creating a sound basis for using this as a design principle for electrically conducting MOFs.