Article,

The weak 3D Topological Insulator Bi$_12$Rh$_3$Sn$_3$I$_9$

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Chem. Eur. J., 26 (67): 15549-15557 (Jun 3, 2020)
DOI: https://doi.org/10.1002/chem.202001953

Abstract

Abstract Topological insulators (TIs) gained high interest due to their protected electronic surface states that allow dissipation-free electron and information transport. In consequence, TIs are recommended as materials for spintronics and quantum computing. Yet, the number of well-characterized TIs is rather limited. To contribute to this field of research, we focused on new bismuth-based subiodides and recently succeeded in synthesizing a new compound Bi12Rh3Sn3I9, which is structurally closely related to Bi14Rh3I9 – a stable, layered material. In fact, Bi14Rh3I9 is the first experimentally supported weak 3D TI. Both structures are composed of well-defined intermetallic layers of ∞2(Bi4Rh)3I2+ with topologically protected electronic edge-states. The fundamental difference between Bi14Rh3I9 and Bi12Rh3Sn3I9 lies in the composition and the arrangement of the anionic spacer. While the intermetallic 2D TI layers in Bi14Rh3I9 are isolated by ∞1Bi2I82− chains, the isoelectronic substitution of bismuth(III) with tin(II) leads to ∞2Sn3I82− layers as anionic spacers. First transport experiments support the 2D character of this material class and revealed metallic conductivity.

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