首页> 外文OA文献 >Effects of octahedral tilting on the electronic structure and optical properties of $d^0$ double perovskites $\mathbf{ m A_2ScSbO_6}$ ($\mathbf{ m A=Sr, Ca}$)
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Effects of octahedral tilting on the electronic structure and optical properties of $d^0$ double perovskites $\mathbf{ m A_2ScSbO_6}$ ($\mathbf{ m A=Sr, Ca}$)

机译:八面体倾斜对电子结构和光学系统的影响   属性$ d ^ 0 $ double perovskites $ \ mathbf {\ rm a_2scsbO_6} $   ($ \ mathbf {\ rm a = sr,Ca} $)

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摘要

With increasing temperature, ${\rm Sr}_2{\rm ScSbO}_6$ undergoes threestructural phase transitions at approximately ${\rm 400K}$, ${\rm 560K}$ and${\rm 650K}$, leading to the following sequence of phases: $P2_1/n \rightarrowI2/m \rightarrow I4/m \rightarrow Fm\bar{3}m$, making it an ideal candidate tostudy the effects of octahedral tilting keeping other parameters fixed. Toascertain the isolated effects of octahedral distortions, the electronic andoptical properties of the monoclinic $P2_1/n$ (at room temperature), monoclinic$I2/m$ (at ${\rm 430K}$), tetragonal $I4/m$ (at ${\rm 613K}$) and the cubic$Fm\bar{3}m$ (at ${\rm 660K}$) phases have been studied in terms of theelectronic structure, dielectric constant, optical conductivity and electronenergy loss spectroscopy using density functional theory. ${\rm Ca}_2{\rmScSbO}_6$, on the other hand, shows only a $P2_1/n$ phase at room temperatureand its properties have been been compared with the corresponding ${\rm Sr}$compound. UV-Vis spectroscopic studies of the optical properties of theroom-temperature phase of these $d^0$ double perovskite have been performed andpresence of large direct bandgap for both the compounds have been reported. Theelectronic bandgaps for the room temperature phases is found to be in goodagreement with the corresponding experimental values obtained using theKubelka-Munk function. Interestingly, in contrast to other Sc-based $d^0$double perovskites, with increasing octahedral distortions, the effective$t_{\rm 2g}$ bandwidth remains unaffected while the states forming the bandchange due to changes in unit cell orientation, leading to small effects on theelectronic and optical properties.
机译:随着温度的升高,$ {\ rm Sr} _2 {\ rm ScSbO} _6 $经历三个结构的相变,分别约为$ {\ rm 400K} $,$ {\ rm 560K} $和$ {\ rm 650K} $。以下阶段顺序:$ P2_1 / n \ rightarrowI2 / m \ rightarrow I4 / m \ rightarrow Fm \ bar {3} m $,使其成为研究八面体倾斜效果并保持其他参数固定的理想选择。为了确定八面体畸变的孤立影响,单斜晶的$ P2_1 / n $(在室温下),单斜晶的$ I2 / m $(在$ {\ rm 430K} $时),四方晶的II / m $(在$ {\ rm 613K} $)和立方$ Fm \ bar {3} m $($ {\ rm 660K} $)相中研究了电子结构,介电常数,光导率和电子能谱使用密度泛函理论另一方面,$ {\ rm Ca} _2 {\ rmScSbO} _6 $在室温下仅显示$ P2_1 / n $相,并且已将其性质与相应的$ {\ rm Sr} $化合物进行了比较。已经对这些$ d ^ 0 $双钙钛矿的室温相的光学性质进行了UV-Vis光谱学研究,并且已经报道了这两种化合物存在大的直接带隙。发现室温相的电子带隙与使用Kubelka-Munk函数获得的相应实验值非常吻合。有趣的是,与其他基于Sc的$ d ^ 0 $双钙钛矿相反,随着八面体畸变的增加,有效的$ t _ {\ rm 2g} $带宽仍然不受影响,而由于晶胞方向的变化而导致能带变化的状态,对电子和光学性能的影响很小。

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