STM studies of candidate topological Kondo insulator SmB<sub>6</sub>
· Invited
Abstract
SmB6 has been proposed a topological Kondo insulator with nontrivial surface states inside a bulk hybridization gap. Experimentally, hybridization between localized 4f and conduction band states at low temperatures is well established [1]. Using STM, we performed local measurements on well identified, atomically flat, unreconstructed surfaces [2]. Tunneling spectroscopy down to 0.35 K revealed sharp peak-like features with a strong temperature dependence within the hybridization gap. The features around –6 mV and –2 mV are dominated by surface contributions to the local density of states [3]. These surface states are robust in the vicinity of randomly occurring non-magnetic impurities, while introducing magnetic impurities in samples (Sm1-xRx)B6 with R = Gd influences the surface states on a much larger length scale compared to non-magnetic impurities [4].
Another material of topical interest is the magnetic Kagome lattice Weyl semimetal Co3Sn2S2 in which time-reversal symmetry breaking causes fascinating physics [5]. The measured local density of states reveals a semimetallic gap of ∼300 mV, verified as the gap in the spin-minority band using spin-resolved tunneling spectra [6].
Work conducted in collaboration with Y. Cheon, C. Felser, C. Guo, G. Li, E. Liu, Y. Sun, L. H. Tjeng, Q. Xu, and H. Yuan.
[1] S. Rößler et al., Proc. Natl. Acad. Sci. USA 111, 4798 (2014).
[2] S. Rößler et al., Phil. Mag. 96, 3262 (2016).
[3] Lin Jiao et al., Nature Commun. 7, 13762 (2016).
[4] Lin Jiao et al., Sci. Adv. 4, eaau4886 (2018).
[5] Enke Liu et al., Nature Phys. 14, 1125 (2018).
[6] Lin Jiao et al., Phys. Rev. B 99, 245158 (2019).
Another material of topical interest is the magnetic Kagome lattice Weyl semimetal Co3Sn2S2 in which time-reversal symmetry breaking causes fascinating physics [5]. The measured local density of states reveals a semimetallic gap of ∼300 mV, verified as the gap in the spin-minority band using spin-resolved tunneling spectra [6].
Work conducted in collaboration with Y. Cheon, C. Felser, C. Guo, G. Li, E. Liu, Y. Sun, L. H. Tjeng, Q. Xu, and H. Yuan.
[1] S. Rößler et al., Proc. Natl. Acad. Sci. USA 111, 4798 (2014).
[2] S. Rößler et al., Phil. Mag. 96, 3262 (2016).
[3] Lin Jiao et al., Nature Commun. 7, 13762 (2016).
[4] Lin Jiao et al., Sci. Adv. 4, eaau4886 (2018).
[5] Enke Liu et al., Nature Phys. 14, 1125 (2018).
[6] Lin Jiao et al., Phys. Rev. B 99, 245158 (2019).
*Financial support from the Deutsche Forschungsgemeinschaft (DFG) through SPP1666 is gratefully acknowledged. Support from the Alexander von Humboldt Foundation and from the Laboratory Directed Research and Development Program of Los Alamos National Laboratory (20160085DR) is acknowledged.
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Presenters
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Steffen Wirth
- Max Planck Institute for Chemical Physics of Solids