A Chemically Triggered and Thermally Switched Dielectric Constant Transition in a Metal Cyanide Based Crystal

A dielectric constant transition is chemically triggered and thermally switched in (HPy)2[Na(H2O)Co(CN)6] (2, HPy=pyridinium cation) by single‐crystal‐to‐single‐crystal transformation and structural phase transition, respectively. Upon dehydration, (HPy)2[Na(H2O)2Co(CN)6] (1) transforms to its semi‐...

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Published inAngewandte Chemie International Edition Vol. 54; no. 21; pp. 6206 - 6210
Main Authors Shi, Chao, Zhang, Xi, Cai, Ying, Yao, Ye-Feng, Zhang, Wen
Format Journal Article
LanguageEnglish
Published Weinheim WILEY-VCH Verlag 18.05.2015
WILEY‐VCH Verlag
Wiley Subscription Services, Inc
EditionInternational ed. in English
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Summary:A dielectric constant transition is chemically triggered and thermally switched in (HPy)2[Na(H2O)Co(CN)6] (2, HPy=pyridinium cation) by single‐crystal‐to‐single‐crystal transformation and structural phase transition, respectively. Upon dehydration, (HPy)2[Na(H2O)2Co(CN)6] (1) transforms to its semi‐hydrated form 2, accompanying a transition from a low‐dielectric state to a high‐dielectric state, and vice versa. This dielectric switch is also realized by a structural phase transition in 2 that occurs between room‐ and low‐temperature phases, and which corresponds to high‐ and low‐dielectric states, respectively. The switching property is due to the variation in the environment surrounding the HPy cation, that is, the hydrogen‐bonding interactions and the crystal packing, which exert predominant influences on the dynamics of the cations that transit between the static and motional states. A dielectric constant transition is observed in (HPy)2[Na(H2O)Co(CN)6] (HPy=pyridinium cation). This transition is chemically triggered by water in a single‐crystal‐to‐single‐crystal transformation (see picture; right) and thermally switched (left) in a structural phase transition.
Bibliography:ArticleID:ANIE201501344
NSFC - No. 21225102; No. 21174039
istex:00680C6FA280CE2EBF26D39F3B6310146C2122DC
ark:/67375/WNG-HMK8JNH2-M
This work was financially supported by the NSFC (Grant No. 21225102 and 21174039). We thank beamline BL14B (Shanghai Synchrotron Radiation Facility) for providing the beam time.
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ISSN:1433-7851
1521-3773
1521-3773
DOI:10.1002/anie.201501344