4.7 Article

Switchable dielectric constant, structural and vibrational studies of double perovskite organic-inorganic hybrids: (azetidinium)2[KCr(CN)6] and (azetidinium)2[KFe(CN)6]

Journal

CRYSTENGCOMM
Volume 24, Issue 27, Pages 4932-4939

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d2ce00270a

Keywords

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Funding

  1. National Science Center (Narodowe Centrum Nauki) in Poland [2021/05/X/ST5/01382]
  2. European Regional Development Fund [POIG.02.01.00-12-023/08]

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We have synthesized and characterized two new organic-inorganic hybrid crystals: AZECr and AZEFe. Thermal analysis results indicate that both compounds undergo a structural phase transition during cooling. Crystal structure analysis shows that AZECr and AZEFe are isomorphous in the high-temperature phase, but differ in the low-temperature phase. Infrared spectroscopy and dielectric measurements confirm the existence of this transition.
We have synthesized and characterized two novel organic-inorganic hybrid crystals: (C3H8N)(2)[KCr(CN)(6)] (AZECr) and (C3H8N)(2)[KFe(CN)(6)] (AZEFe). Thermal DSC, TG and DT analyses indicate that each compound undergoes one structural phase transition (PT). AZECr and AZEFe undergo a structural phase transition each upon cooling at 171 and 186 K, respectively. The crystal structures are refined for AZECr-high-temperature, AZECr-low-temperature, and AZEFe-high-temperature at 210 K, 120, and 240 K, respectively. AZECr and AZEFe are isomorphous at the high-temperature (HT) phase and are characterized by a three-dimensional framework consisting of [X4K4(CN)(12)] (where X are Cr-III or Fe-III) cages formed by X-C N-K fragments, which are filled by guest azetidinium (AZE(+)) cations. The crystal system changes during the PT in AZECr from the HT phase to the low-temperature (LT) phase, as shown at 120 K, where the crystal adopts the P2(1)/c monoclinic space group. The AZE(+) cations and the CN- bridges, which were highly disordered in the HT phase, are fully ordered in the LT one. AZEFe-LT diffraction data reveal extensive twinning of the crystal, and, unfortunately, our attempts to solve the structure of the crystal were unsuccessful. To compare and obtain insight into the mechanisms of PTs in these crystals, we measured the infrared (IR) spectra in a wide wavenumber range from middle IR (MIR) to far IR (FIR). IR measurements fully confirm that both samples are isomorphous at the HT phase. However, in the LT phase, the spectra are different, which means that the LT phases are not identical and may suggest that AZECr-LT and AZEFe-LT are not isomorphous. Additionally, to confirm the change in dynamical states of molecules in PT, dielectric measurements were carried out between 150 and 300 K in the frequency range of 25 Hz to 2 MHZ. It was shown that the permittivity value can be switched between two states: ON (a high epsilon ' value, HT) and OFF (a low epsilon' value, LT).

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