Taouti Mohamed B, Suffren Yan, Leynaud Olivier, Benbertal Djamal, Brenier Alain, Gautier-Luneau Isabelle
†Institut NEEL, Université Grenoble Alpes, F-38042 Grenoble, France.
‡CNRS, Institut NEEL, F-38042 Grenoble, France.
Inorg Chem. 2015 Apr 6;54(7):3608-18. doi: 10.1021/acs.inorgchem.5b00187. Epub 2015 Mar 19.
The structural and thermal studies of six anhydrous lanthanum iodate polymorphs are presented. The variation of the [IO3(-)]:[La(3+)] molar ratio in the starting solution and the evaporation rate of the solution leads to either the centric La(IO3)3(HIO3) or the acentric La(IO3)3(HIO3)1.33 phases. The crystal structure of La(IO3)3(HIO3)1.33 was determined. The thermal treatments of these two phases up to 490 °C lead to β-La(IO3)3, observed at room temperature. To better understand the similar thermal behaviors of La(IO3)3(HIO3)1.33 and La(IO3)3(HIO3) compounds and their structural evolution, thermogravimetry-differential thermal analysis (TG-DTA), differential scanning calorimetry (DSC) analyses and in situ temperature-dependent powder X-ray diffraction (XRD) experiments were carried out. These experiments allowed us to highlight the successive formation of δ-La(IO3)3 and γ-La(IO3)3. δ-La(IO3)3 is observed from the beginning of thermal decomposition of La(IO3)3(HIO3)1.33 (at 340 °C) or La(IO3)3(HIO3) (at 300 °C) up to 440 °C. A phase transition from δ-La(IO3)3 to γ-La(IO3)3 then occurs at 440 °C. Finally, the phase transition from γ-La(IO3)3 to β-La(IO3)3 occurs at 140 °C. A cycle of heating and cooling shows the reversible phase transition at 185 and 140 °C, respectively. β-, γ-, and δ-La(IO3)3 are three polymorph phases of the first α-La(IO3)3 already characterized. The structure of β-La(IO3)3 and γ-La(IO3)3 were determined on powder XRD analyses. The iodate compounds present a very broad domain of transparency from the visible range to the beginning of the far-infrared range. The intensities of SHG light generated by α-La(IO3)3, β-La(IO3)3, La(IO3)3(HIO3)1.33, and α-LiIO3 compounds with acentric structures were compared: β-La(IO3)3 < La(IO3)3(HIO3)1.33 < α-La(IO3)3 ≈ α-LiIO3. Finally, the luminescence spectroscopy of La(IO3)3(HIO3)1.33:Nd(3+), α-La(IO3)3:Nd(3+), and α-La(IO3)3:Yb(3+) is studied.
本文介绍了六种无水碘酸镧多晶型物的结构和热学研究。起始溶液中[IO₃⁻]:[La³⁺]摩尔比的变化以及溶液的蒸发速率会导致形成中心对称的La(IO₃)₃(HIO₃)或非中心对称的La(IO₃)₃(HIO₃)₁.₃₃相。确定了La(IO₃)₃(HIO₃)₁.₃₃的晶体结构。对这两种相在高达490℃的温度下进行热处理,会得到室温下观察到的β-La(IO₃)₃。为了更好地理解La(IO₃)₃(HIO₃)₁.₃₃和La(IO₃)₃(HIO₃)化合物相似的热行为及其结构演变,进行了热重-差示热分析(TG-DTA)、差示扫描量热法(DSC)分析以及原位变温粉末X射线衍射(XRD)实验。这些实验使我们能够突出δ-La(IO₃)₃和γ-La(IO₃)₃的相继形成。从La(IO₃)₃(HIO₃)₁.₃₃(在340℃)或La(IO₃)₃(HIO₃)(在300℃)开始热分解直至440℃,都能观察到δ-La(IO₃)₃。然后在440℃发生从δ-La(IO₃)₃到γ-La(IO₃)₃的相变。最后,在140℃发生从γ-La(IO₃)₃到β-La(IO₃)₃的相变。加热和冷却循环分别显示在185℃和140℃发生可逆相变。β-La(IO₃)₃、γ-La(IO₃)₃和δ-La(IO₃)₃是已表征的第一种α-La(IO₃)₃的三种多晶型相。通过粉末XRD分析确定了β-La(IO₃)₃和γ-La(IO₃)₃的结构。碘酸盐化合物在从可见光范围到远红外范围起始部分呈现出非常宽的透明域。比较了具有非中心对称结构的α-La(IO₃)₃、β-La(IO₃)₃、La(IO₃)₃(HIO₃)₁.₃₃和α-LiIO₃化合物产生SHG光的强度:β-La(IO₃)₃ < La(IO₃)₃(HIO₃)₁.₃₃ < α-La(IO₃)₃ ≈ α-LiIO₃。最后,研究了La(IO₃)₃(HIO₃)₁.₃₃:Nd³⁺、α-La(IO₃)₃:Nd³⁺和α-La(IO₃)₃:Yb³⁺的发光光谱。