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在砷化镓上外延生长的少五层拓扑绝缘体Bi2Se3薄膜的低温拉曼指纹图谱。

Low-temperature Raman fingerprints for few-quintuple layer topological insulator Bi2Se3 films epitaxied on GaAs.

作者信息

Eddrief Mahmoud, Atkinson Paola, Etgens Victor, Jusserand Bernard

机构信息

Sorbonne Universités, UPMC Université Paris 6, UMR 7588, Institut des NanoSciences de Paris, 4 Place Jussieu, F-75005 Paris, France. CNRS, UMR 7588, Institut des NanoSciences de Paris, 4 Place Jussieu, F-75005 Paris, France.

出版信息

Nanotechnology. 2014 Jun 20;25(24):245701. doi: 10.1088/0957-4484/25/24/245701. Epub 2014 May 23.

Abstract

Topological insulators (Bi2Se3) of single- and few-quintuple-layer (few-QLs) films were investigated by Raman spectroscopy and epitaxied on a GaAs substrate. At a measurement temperature of 80 K, we observed the emergence of additional A2u and Eu modes (Raman inactive in the bulk crystal) below 9-QLs film thicknesses, assigned to the crystal-symmetry breakdown in ultrathin films. Furthermore, the out-of-plane A1g modes changed in width, frequency, and intensity for decreasing numbers of QL, while the in-plane Eg mode split into three Raman lines, not resolved in previous room temperature experiments. The out-of-plane Raman modes showed a strong Raman resonance at 2.4 eV for around 4-QLs film thickness, and the resonant position of the same modes shifted to 2.2 eV for 18-QLs-thick film. The film thickness-dependence of the phonons frequencies cannot solely be explained within models of weak van der Waals interlayer coupling. The results are discussed in terms of stacking-induced changes in inter- and intralayer bonding and/or the presence of long-range Coulombic interlayer interactions in topological insulator Bi2Se3. This work demonstrates that Raman spectroscopy is sensitive to changes in film thickness over the critical range of 9- to 4-QLs, which coincides with the transition between a gapless topological insulator (occurring above 6-QLs) to a conventional gapped insulator (occurring below 4-QLs).

摘要

通过拉曼光谱对单重和少数五重层(少数QLs)的拓扑绝缘体(Bi2Se3)薄膜进行了研究,并将其外延生长在GaAs衬底上。在80K的测量温度下,我们观察到在薄膜厚度小于9QLs时出现了额外的A2u和Eu模式(在体晶体中拉曼非活性),这归因于超薄薄膜中的晶体对称性破坏。此外,面外A1g模式的宽度、频率和强度随QL数量的减少而变化,而面内Eg模式分裂为三条拉曼线,这在之前的室温实验中未得到分辨。面外拉曼模式在薄膜厚度约为4QLs时在2.4eV处显示出强烈的拉曼共振,对于18QLs厚的薄膜,相同模式的共振位置移至2.2eV。声子频率的薄膜厚度依赖性不能仅用弱范德华层间耦合模型来解释。根据拓扑绝缘体Bi2Se3中堆叠引起的层间和层内键合变化和/或长程库仑层间相互作用的存在对结果进行了讨论。这项工作表明,拉曼光谱对9至4QLs临界范围内的薄膜厚度变化敏感,这与无隙拓扑绝缘体(发生在6QLs以上)到传统带隙绝缘体(发生在4QLs以下)的转变相一致。

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