Eddrief Mahmoud, Atkinson Paola, Etgens Victor, Jusserand Bernard
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.
Nanotechnology. 2014 Jun 20;25(24):245701. doi: 10.1088/0957-4484/25/24/245701. Epub 2014 May 23.
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).
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。