Topological Insulator Thin Films Starting from the Amorphous Phase - BiSe as Example
arXiv:1502.01135 · doi:10.1063/1.4908007
Abstract
We present a new method to obtain topological insulator BiSe thin films with a centimeter large lateral length. To produce amorphous BiSe thin films we have used a sequential flash-evaporation method at room temperature. Transmission electron microscopy has been used to verify that the prepared samples are in a pure amorphous state. During annealing the samples transform into the rhombohedral BiSe crystalline strcuture which was confirmed using X-ray diffraction and Raman spectroscopy. Resistance measurements of the amorphous films show the expected Mott variable range hopping conduction process with a high specific resistance compared to the one obtained in the crystalline phase (metallic behavior). We have measured the magnetoresistance (MR) and the Hall effect (HE) at different temperatures between 2 K and 275 K. At temperatures K and fields T we observe weak anti-localization in the MR; the Hall measurements confirm the n-type character of the samples. All experimental results of our films are in quantitative agreement with results from samples prepared using more sophisticated methods.
8 pages, 9 figures, to be published in Journal of Applied Physics (2015)
References in corpus (8)
- Quantum Spin Hall Insulator State in HgTe Quantum Wells
- Discovery (theoretical prediction and experimental observation) of a large-gap topological-insulator class with spin-polarized single-Dirac-cone on the surface
- First direct observation of Spin-textures in Topological Insulators : Spin-resolved ARPES as a probe of topological quantum spin Hall effect and Berry's phase
- Surface States of the Topological Insulator Bi_{1-x}Sb_x
- Gate-Voltage Control of Chemical Potential and Weak Anti-localization in Bismuth Selenide
- Bulk Fermi surface coexistence with Dirac surface state in BiSe: a comparison of photoemission and Shubnikov-de Haas measurements
- Impurity effect on weak anti-localization in the topological insulator Bi2Te3
- Topological delocalization of two-dimensional massless Dirac fermions