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    Determination of charge ordering pattern of the organic salt α′−(ET)2IBr2 using x-ray diffraction

    Dongho Yoon1, Hiromi Taniguchi2, Takuya Kobayashi2,3, Kiyonori Takahashi4,5,6, Shuhei Fukuoka1, and Atsushi Kawamoto1

    • 1Department of Condensed Matter Physics, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan
    • 2Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan
    • 3Research and Development Bureau, Saitama University, Saitama 338-8570, Japan
    • 4Graduate School of Environmental Science, Hokkaido University, Sapporo 060-0810, Japan
    • 5Research Institute for Electronic Science, Hokkaido University, Sapporo 010-0020, Japan
    • 6Faculty of Advanced Science and Technology, Kumamoto University, Kumamoto 860-8555, Japan

    Phys. Rev. B 113, 064103 – Published 4 February, 2026

    DOI: https://doi.org/10.1103/f7hw-7436

    Abstract

    Single-crystal x-ray diffraction (XRD) measurements were conducted on quasi-two-dimensional organic salt α′−(ET)2IBr2 to investigate the charge ordering (CO) pattern, which remained unresolved by local probes, and the anomalous absence of second-harmonic generation (SHG) signal at intermediate temperature (160K<T<200K). Our structural analysis at 110 K reveals a noncentrosymmetric horizontal stripe type CO pattern with a charge separation (Δρ=|ρrich−ρpoor|) of Δρ≈0.8e. These findings are consistent with results from C−NMR13, vibrational spectroscopy, and the observation of finite SHG signal. At intermediate temperature, SHG signal was absent despite the presence of CO, indicating a superstructure with antiparallel polarization. However, there was no direct structural evidence, including phase transition and CO pattern at 200 K. A superlattice structure with lattice doubling along the c axis was identified in the intermediate temperature range (160K<T<200K). The structural analysis at 180 K confirms that the charge ordered layers are related by an inversion center and exhibit a horizontal stripe type CO pattern, explaining the absence of SHG signal in this phase. Those findings establish three distinct structural and electronic phases in α′−(ET)2IBr2. Furthermore, the suppression of dynamic ethylene group disorder below 200 K was observed, suggesting a possible contribution to the previously reported Raman spectral broadening of the anion. This offers an alternative explanation to the previous model based on dynamic charge fluctuations.

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