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Vacuum Interfacial Structure and X‑ray Reflectivity of Imidazolium-Based Ionic Liquids with Perfluorinated Anions from a Theory and Simulations Perspective
Journal article   Open access   Peer reviewed

Vacuum Interfacial Structure and X‑ray Reflectivity of Imidazolium-Based Ionic Liquids with Perfluorinated Anions from a Theory and Simulations Perspective

Waruni V. Karunaratne, Man Zhao, Edward W. Castner and Claudio J. Margulis
Journal of physical chemistry. C, Vol.126(32), pp.13936-13945
08/18/2022
DOI: 10.1021/acs.jpcc.2c03311
url
https://doi.org/10.1021/acs.jpcc.2c03311View
Published (Version of record) Open Access

Abstract

We report studies of the vacuum interfacial structure of a series of 1-methyl-3-alkylimidazolium bis­(perfluoro­alkanesulfonyl)­imide ionic liquids (ILs) and predict and explain their Fresnel-normalized X-ray reflectivity. To better interpret the results, we use a theory we recently developed dubbed “the peaks and antipeaks analysis of reflectivity” which splits the overall signal into that of different pair subcomponents. Whereas the overall reflectivity signal is not very informative, the peak and trough intensities for the pair subcomponents provide rich information for analysis. When species containing cationic alkyl or anionic fluoroalkyl tails are present at the interface, a tail layer is found next to a vacuum, and this tail layer can be composed of both alkyl and fluoroalkyl moieties. To maintain the positive–negative alternation of charged groups, alkyl and fluoroalkyl tails must necessarily be nearby and cannot segregate. Charged groups are found in the subsequent layer just below the interface and arranged to achieve lateral charge neutrality. In general, fluctuations at and away from the interface are based on polarity (i.e., heads and tails) and not on charge; when there are no significant alkyl or fluoroalkyl moieties in the IL, atomic density fluctuations away from the interface are small and appear to exist for the purpose of achieving lateral charge balance. For all the systems reported here, the persistence length of density fluctuations does not go beyond ∼7 nm.
C: Physical Properties of Materials and Interfaces UIOWA OA Agreement

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