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Origin of the low critical observing temperature of the quantum anomalous Hall effect in V-doped (Bi, Sb)(2)Te(3) film

The experimental realization of the quantum anomalous Hall (QAH) effect in magnetically-doped (Bi, Sb)(2)Te(3) films stands out as a landmark of modern condensed matter physics. However, ultra-low temperatures down to few tens of mK are needed to reach the quantization of Hall resistance, which is t...

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Detalles Bibliográficos
Autores principales: Li, W., Claassen, M., Chang, Cui-Zu, Moritz, B., Jia, T., Zhang, C., Rebec, S., Lee, J. J., Hashimoto, M., Lu, D.-H., Moore, R. G., Moodera, J. S., Devereaux, T. P., Shen, Z.-X.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5013448/
https://www.ncbi.nlm.nih.gov/pubmed/27599406
http://dx.doi.org/10.1038/srep32732
Descripción
Sumario:The experimental realization of the quantum anomalous Hall (QAH) effect in magnetically-doped (Bi, Sb)(2)Te(3) films stands out as a landmark of modern condensed matter physics. However, ultra-low temperatures down to few tens of mK are needed to reach the quantization of Hall resistance, which is two orders of magnitude lower than the ferromagnetic phase transition temperature of the films. Here, we systematically study the band structure of V-doped (Bi, Sb)(2)Te(3) thin films by angle-resolved photoemission spectroscopy (ARPES) and show unambiguously that the bulk valence band (BVB) maximum lies higher in energy than the surface state Dirac point. Our results demonstrate clear evidence that localization of BVB carriers plays an active role and can account for the temperature discrepancy.