Almgren J, Streltsov VA, Sobolev AN, Figgis BN, Albertsson J
Inorganic Chemistry, Chalmers University of Technology, SE-412 96 Göteborg, Sweden.
Acta Crystallogr B. 1999 Oct 1;55(Pt 5):712-720. doi: 10.1107/s010876819900395x.
Structure factors for rubidium titanyl arsenate, RbTiOAsO(4), were measured with Mo Kalpha radiation (lambda = 0.71069 Å) at 9.6 and 295 K. The data show that there is no phase transition between room temperature and 9.6 K. The space group is Pna2(1). Unit-cell parameters are a = 13.218 (1), b = 6.6500 (9) and c = 10.761 (1) Å at 9.6 K, and a = 13.261 (2), b = 6.6791 (8) and c = 10.769 (1) Å at 295 K. As the temperature was lowered from 295 to 9.6 K the Rb atoms moved along the c axis in the direction of the polarization vector, while no significant change was noted for the Ti-O-As network. Strong accumulation and polarization of the difference electron density (Deltarho) in exceptionally short covalent Ti-O bonds alternates with the depleted density in long Ti-O bonds. The Deltarho near the Ti atoms is polarized and aligned in the negative c direction in accordance with the ferroelectric properties of this material. However, the electron density near the Rb atoms is depleted in this direction and the excess Deltarho is moved further away from the nuclei along the c vector.
采用钼Kα辐射(λ = 0.71069 Å)在9.6 K和295 K温度下测量了砷酸钛氧铷(RbTiOAsO₄)的结构因子。数据表明,在室温至9.6 K之间没有相变。空间群为Pna2(1)。9.6 K时的晶胞参数为a = 13.218 (1) Å、b = 6.6500 (9) Å和c = 10.761 (1) Å,295 K时的晶胞参数为a = 13.261 (2) Å、b = 6.6791 (8) Å和c = 10.769 (1) Å。当温度从295 K降至9.6 K时,Rb原子沿c轴朝着极化矢量方向移动,而Ti - O - As网络没有明显变化。在异常短的共价Ti - O键中,差分电子密度(Δρ)强烈积累和极化,与长Ti - O键中的耗尽密度交替出现。Ti原子附近的Δρ根据该材料的铁电特性在负c方向极化并排列。然而,Rb原子附近的电子密度在这个方向上耗尽,多余的Δρ沿着c矢量进一步远离原子核。