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Crystal structure, phase transition and ferroelectric properties of the [(CH3)3NH]3[Sb2Cl9(1−x)Br9x] (TMACBA) mixed crystals

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Published 8 August 2003 Published under licence by IOP Publishing Ltd
, , Citation M Wojtaś et al 2003 J. Phys.: Condens. Matter 15 5765 DOI 10.1088/0953-8984/15/33/310

0953-8984/15/33/5765

Abstract

The paraelectric–ferroelectric phase transition in the [(CH3)3NH]3[Sb2Cl9(1−x) Br9x]  (TMACBA) mixed crystals is investigated by the differential scanning calorimetry, dilatometric and dielectric methods. The phase transition is found at 363.5, 362.7, 360.5 and 350.9 K (on cooling) for TMACBA crystals with x = 0, 0.02, 0.17 and 0.42, respectively. The crystal structures of the pure bromine analogue (x = 1), TMABA, and the mixed crystal TMACBA (x = 0.55) are determined at 297 K. TMABA crystallizes in the trigonal space group Rbar 3ca = 15.098(2) Å, c = 21.906(4) Å, Z = 3, R1 = 0.0393, wR2 = 0.0746. Its structure is built up of discrete Sb2Br93− bioctahedra and disordered trimethylammonium cations. Ferroelectric TMACBA (x = 0.55) crystallizes in the monoclinic space group Pc: a = 10.245(2) Å, b = 9.122(2) Å, c = 15.549(3) Å, β = 90.52(3)°, Z = 2, R1 = 0.0340, wR2 = 0.0712. The crystal is built of two-dimensional layer anions ('honeycomb-like structure') and three trimethylammonium cations. Dielectric studies on TMACBA (x = 0.42) in the frequency range 75 kHz–900 MHz indicate relatively fast reorientation of the trimethylammonium cations over the paraelectric phase. The ferroelectricity of mixed crystals is preserved for Br concentration smaller than 0.60 ± 0.05. The polar properties are strictly connected with the presence of the polyanionic layer structure. A possible mechanism for the paraelectric–ferroelectric phase transition in the TMACBA mixed crystals is discussed on the basis of the results presented.

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10.1088/0953-8984/15/33/310