Departamento de Química, Universidade Federal de Ouro Preto, Campus Morro do Cruzeiro, ICEB II, Sala 67, Ouro Preto-MG, 35400-000, Brazil.
Dalton Trans. 2011 Oct 7;40(37):9454-60. doi: 10.1039/c1dt10783f. Epub 2011 Aug 18.
Lanthanide orthotantalates RETaO(4) (RE = La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, and Lu) were synthesized by solid-state reaction in optimized conditions of temperature (1300 °C) and time (up to 14 h) to yield crystalline materials. The crystal structures of the obtained compounds were investigated by X-ray diffraction and Raman scattering. All the samples exhibited monoclinic structures, but with different arrangements as a function of the ionic radius of the rare-earth metal occupying the A-site. For compounds with the largest ionic radii (La-Pr), the ceramics crystallized in the monoclinic structure, P2(1)/c (C(2h)(5), #14, Z = 4), while the compounds with intermediate ionic radii (Nd-Tb) exhibited the fergusonite M-type structure, I2/a (C(2h)(6), #15, Z = 4). Samples with the smallest ionic radii (Dy-Lu) presented the fergusonite M'-type structure, P2/a (C(2h)(4), #13, Z = 2). These last two groups of compounds exhibited phase transitions, which can be related to the processing temperature. The compounds belonging to the M-type structure are stable at high temperatures, whilst materials belonging to the M'-type structure are stable at low temperatures. The results from XRD and Raman scattering allows us to understand the differences between these two structures in terms of the vibrational-active modes assigned to each space group. Also, the Raman patterns in addition to group-theory calculations for this complete lanthanide series were reported for the first time. The experimental results are in perfect agreement with theoretical calculations: samples with P2(1)/c (#14) structure showed 36 Raman-active modes, while both I2/a (#15) and P2/a (#13) structures exhibited 18 Raman modes.
镧系 orthotantalates RETaO(4)(RE = La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb 和 Lu)通过固态反应在温度(1300°C)和时间(最长 14 小时)的优化条件下合成,以生成结晶材料。通过 X 射线衍射和拉曼散射研究了所得化合物的晶体结构。所有样品均表现出单斜结构,但随着占据 A 位的稀土金属离子半径的不同,其排列方式也不同。对于具有最大离子半径(La-Pr)的化合物,陶瓷在单斜结构 P2(1)/c(C(2h)(5),#14,Z = 4)中结晶,而具有中等离子半径(Nd-Tb)的化合物表现出 Fergusonite M 型结构,I2/a(C(2h)(6),#15,Z = 4)。具有最小离子半径(Dy-Lu)的样品呈现 Fergusonite M'-型结构,P2/a(C(2h)(4),#13,Z = 2)。这最后两组化合物表现出相变,这可以与处理温度相关。属于 M 型结构的化合物在高温下稳定,而属于 M'-型结构的化合物在低温下稳定。XRD 和拉曼散射的结果允许我们根据每个空间群分配的振动活性模式来理解这两种结构之间的差异。此外,还首次报道了该完整镧系元素系列的拉曼图谱以及群论计算。实验结果与理论计算完全吻合:具有 P2(1)/c(#14)结构的样品显示 36 个拉曼活性模式,而 I2/a(#15)和 P2/a(#13)结构均显示 18 个拉曼模式。