Volume 19, Issue 12 p. 1441-1447
Article

Long Periodic Structure of a Room‐Temperature Ionic Liquid by High‐Pressure Small‐Angle X‐Ray Scattering and Wide‐Angle X‐Ray Scattering: 1‐Decyl‐3‐Methylimidazolium Chloride

Dr. Hiroshi Abe

Corresponding Author

Department of Materials Science and Engineering, National Defense Academy, Yokosuka, 239-8686 Japan

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Nozomu Hamaya

Graduate School of Humanities and Sciences, Ochanomizu University, Tokyo, 112-8610 Japan

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Yoshihiro Koyama

Graduate School of Pure and Applied Science, University of Tsukuba, Tsukuba, 305-8573 Japan

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Hiroaki Kishimura

Department of Materials Science and Engineering, National Defense Academy, Yokosuka, 239-8686 Japan

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Takahiro Takekiyo

Department of Applied Chemistry, National Defense Academy, Yokosuka, 239-8686 Japan

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Yukihiro Yoshimura

Department of Applied Chemistry, National Defense Academy, Yokosuka, 239-8686 Japan

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Daisuke Wakabayashi

Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, 305-0801 Japan

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Nobumasa Funamori

Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, 305-0801 Japan

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Kiyoto Matsuishi

Graduate School of Pure and Applied Science, University of Tsukuba, Tsukuba, 305-8573 Japan

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First published: 23 April 2018
Citations: 7

Abstract

The Bragg reflections of 1‐decyl‐3‐methylimidazolium chloride ([C10mim][Cl]), a room‐temperature ionic liquid, are observed in a lowly scattered wavevector (q) region using high‐pressure (HP) small‐angle X‐ray scattering methods. The HP crystal of [C10mim][Cl] was characterized by an extremely long periodic structure. The peak position at the lowest q (1.4 nm−1) was different from that of the prepeak observed in the liquid state (2.3 nm−1). Simultaneously, Bragg reflections at high‐q were detected using HP wide‐angle X‐ray scattering. The longest lattice constant was estimated to be 4.3 nm using structural analysis. The crystal structure of HP differed from that of the low‐temperature (LT) crystal and the LT liquid crystal. With increasing pressure, Bragg reflections in the high‐q component became much broader, and were accompanied by phase transition, although those in the low‐q component were observed to be relatively sharp.