Direct observation of the spin texture in strongly correlated SmB6 as evidence of the topological Kondo insulator
Autor: | Xu, N., Biswas, P. K., Dil, J. H., Dhaka, R. S., Landolt, G., Muff, S., Matt, C. E., Shi, X., Plumb, N. C., Radovic, M., Pomjakushina, E., Conder, K., Amato, A., Borisenko, S. V., Yu, R., Weng, H. -M., Fang, Z., Dai, X., Mesot, J., Ding, H., Shi, M. |
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Rok vydání: | 2014 |
Předmět: | |
Zdroj: | Nature Communications 5:4566 (2014) |
Druh dokumentu: | Working Paper |
DOI: | 10.1038/ncomms5566 |
Popis: | The concept of a topological Kondo insulator (TKI) has been brought forward as a new class of topological insulators in which non-trivial surface states reside in the bulk Kondo band gap at low temperature due to the strong spin-orbit coupling [1-3]. In contrast to other three-dimensional (3D) topological insulators (e.g. Bi2Se3), a TKI is truly insulating in the bulk [4]. Furthermore, strong electron correlations are present in the system, which may interact with the novel topological phase. Applying spin- and angle-resolved photoemission spectroscopy (SARPES) to the Kondo insulator SmB6, a promising TKI candidate, we reveal that the surface states of SmB6 are spin polarized, and the spin is locked to the crystal momentum. Counter-propagating states (i.e. at k and -k) have opposite spin polarizations protected by time-reversal symmetry. Together with the odd number of Fermi surfaces of surface states between the 4 time-reversal invariant momenta in the surface Brillouin zone [5], these findings prove, for the first time, that SmB6 can host non-trivial topological surface states in a full insulating gap in the bulk stemming from the Kondo effect. Hence our experimental results establish that SmB6 is the first realization of a 3D TKI. It can also serve as an ideal platform for the systematic study of the interplay between novel topological quantum states with emergent effects and competing order induced by strongly correlated electrons. Comment: 4 figures |
Databáze: | arXiv |
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