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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Electronic structures of hexagonal RMnO_3 (R=Gd, Tb, Dy, and Ho) thin films: Optical spectroscopy and first-principles calculations
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Electronic structures of hexagonal RMnO_3 (R=Gd, Tb, Dy, and Ho) thin films: Optical spectroscopy and first-principles calculations

机译:六角形RMnO_3(R = Gd,Tb,Dy和Ho)薄膜的电子结构:光谱学和第一性原理计算

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摘要

We investigated the electronic structure of multiferroic hexagonal RMnO_3 (R=Gd, Tb, Dy, and Ho) thin films using both optical spectroscopy and first-principles calculations. One of the difficulties in explaining the electronic structures of hexagonal RMnO_3 is that they exist in nature with limited rare earth ions (i.e., R=Sc, Y, and Ho-Lu), so a systematic study in terms of the different R ions has been lacking. Recently, our group succeeded in fabricating hexagonal RMnO_3 (R=Gd, Tb, and Dy) using the epitaxial stabilization technique [Adv. Mater. (Weinheim Ger.) 18, 3125 (2006)]. Using artificially stabilized hexagonal RMnO_3, we extended the optical spectroscopic studies on the hexagonal multiferroic manganite system. We observed two optical transitions located near 1.7 and 2.3 eV, in addition to the predominant absorption above 5 eV. With the help of first-principles calculations, we attributed the low-lying optical absorption peaks to interband transitions from the oxygen states hybridized strongly with different Mn orbital symmetries to the Mn 3d_(3z~2-r~2) state. As the ionic radius of the rare earth ion increased, we observed a systematic increase of the lowest peak position, which became more evident when compared with previously reported results. We explained this systematic change in terms of a flattening of the MnO_5 triangular bipyramid.
机译:我们使用光谱学和第一性原理计算研究了六方RMnO_3(R = Gd,Tb,Dy和Ho)多铁性薄膜的电子结构。解释六方RMnO_3的电子结构的困难之一是它们存在于自然界中,稀土离子有限(即R = Sc,Y和Ho-Lu),因此对不同R离子的系统研究一直缺乏。最近,我们的小组成功地使用外延稳定技术制造了六角形RMnO_3(R = Gd,Tb和Dy)。母校(Weinheim Ger。)18,3125(2006)]。使用人工稳定的六角形RMnO_3,我们扩展了六角形多铁锰矿体系的光谱研究。除了在5 eV以上的主要吸收外,我们还观察到两个光学跃迁位于1.7和2.3 eV附近。借助第一性原理的计算,我们将低层的光吸收峰归因于带间跃迁,该跃迁是从具有与不同Mn轨道对称性强烈杂交的氧态到Mn 3d_(3z〜2-r〜2)态的带间跃迁。随着稀土离子的离子半径的增加,我们观察到最低峰位置的系统增加,与先前报道的结果相比,这一点更加明显。我们根据MnO_5三角双锥体的扁平化解释了这种系统的变化。

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