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Structure of and electron density in RbTiOAsO4 at 9.6 K

机译:RbTiOAsO4在9.6 K下的结构和电子密度

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Structure factors for rubidium titanyl arsenate, RbTiOAsO4, were measured with Mo K alpha radiation (lambda = 0.71069 Angstrom) 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) Angstrom at 9.6 K, and a = 13.261 (2), b = 6.6791 (8) and c = 10.769 (1) Angstrom at 295 It. 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 (Delta p) in exceptionally short covalent Ti-O bonds alternates with the depleted density in long Ti-O bonds. The Delta rho 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 Delta rho is moved further away from the nuclei along the c vector. [References: 34]
机译:钼tit钛酸钡RbTiOAsO4的结构因子在9.6和295 K时用Mo K alpha辐射(λ= 0.71069埃)测量。数据显示,室温和9.6 K之间没有相变。空间群是Pna2( 1)。晶胞参数为9.6 K时a = 13.218(1),b = 6.6500(9)和c = 10.761(1)埃,以及a = 13.261(2),b = 6.6791(8)和c = 10.769(1 )295 It。当温度从295 K降低到9.6 K时,Rb原子沿c轴在极化矢量的方向上移动,而Ti-O-As网络没有明显变化。在非常短的共价Ti-O键中,差电子密度(Delta p)的强积累和极化与在长Ti-O键中的耗尽密度交替。根据该材料的铁电特性,靠近Ti原子的Δrho极化并沿负c方向排列。但是,Rb原子附近的电子密度在该方向上耗尽,多余的Delta rho沿c向量进一步远离原子核。 [参考:34]

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