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Pressure-induced liquid-liquid transition in a family of ionic materials

Liquid−liquid transition (LLT) between two disordered phases of single-component material remains one of the most intriguing physical phenomena. Here, we report a first-order LLT in a series of ionic liquids containing trihexyl(tetradecyl)phosphonium cation [P(666,14)](+) and anions of different siz...

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Detalles Bibliográficos
Autores principales: Wojnarowska, Zaneta, Cheng, Shinian, Yao, Beibei, Swadzba-Kwasny, Malgorzata, McLaughlin, Shannon, McGrogan, Anne, Delavoux, Yoan, Paluch, Marian
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8924164/
https://www.ncbi.nlm.nih.gov/pubmed/35292645
http://dx.doi.org/10.1038/s41467-022-29021-0
Descripción
Sumario:Liquid−liquid transition (LLT) between two disordered phases of single-component material remains one of the most intriguing physical phenomena. Here, we report a first-order LLT in a series of ionic liquids containing trihexyl(tetradecyl)phosphonium cation [P(666,14)](+) and anions of different sizes and shapes, providing an insight into the structure-property relationships governing LLT. In addition to calorimetric proof of LLT, we report that ion dynamics exhibit anomalous behavior during the LLT, i.e., the conductivity relaxation times (τ(σ)) are dramatically elongated, and their distribution becomes broader. This peculiar behavior is induced by isobaric cooling and isothermal compression, with the τ(σ)(T(LL),P(LL)) constant for a given system. The latter observation proves that LLT, in analogy to liquid-glass transition, has an isochronal character. Finally, the magnitude of discontinuity in a specific volume at LLT was estimated using the Clausius-Clapeyron equation.