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Emergence of -s,-p-d band inversion in zincblende Gold Iodide Topological Insulator and it's Thermoelectric Properties

We employ first-principles calculations to investigate the Topological States (TS) and Thermoelectric (TE) transport properties of three dimensional (3D) Gold Iodide (AuI) which belongs to the zincblende family. We explore, Semi-Metal (SM) to Topological Conductor (TC) and Topological Insulator (TI)...

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Bibliographic Details
Published in:Journal of physics. Condensed matter 2021-04, Vol.33 (15), p.155402
Main Authors: Sattigeri, Raghottam M, Gajaria, Trupti K, Jha, Prafulla K, Spiewak, Piotr, Kurzydłowski, Krzysztof J
Format: Article
Language:English
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Summary:We employ first-principles calculations to investigate the Topological States (TS) and Thermoelectric (TE) transport properties of three dimensional (3D) Gold Iodide (AuI) which belongs to the zincblende family. We explore, Semi-Metal (SM) to Topological Conductor (TC) and Topological Insulator (TI) phase transitions. Under pristine conditions, AuI exhibits Dirac SM nature but, under the influence of mild isotropic compressive pressure the system undergoes electronic quantum phase transition driving it into non-trivial topological state. This state exhibits Dresselhaus like band spin splitting leading to a TC state. In order to realize TI state from the SM state, we break the cubic symmetry of the system by introducing a compressive pressure along (001) crystal direction. The non-trivial TI nature of the system is characterized by the emergence of robust surface states and the Z invariant ν = 1 which indicates a strong TI nature. A novel facet of the phase transition discussed here is, the -s and -p,-d orbital band inversion mechanism which is unconventional as compared to previously explored TI families. This mechanism unravels new path by which TI materials can be predicted. Also, we investigated the lattice and electronic contributions to the TE transport properties. We characterize the TE performance by calculating the Figure of Merit (zT) and find that, at room temperature (300 K) and for a fixed doping concentration (i.e., n = 1×10 cm ) the zT is 0.55 and 0.53 for electrons and holes respectively. This is quite remarkable since, higher values of zT are generally predicted at higher temperature scales whereas, zT values as in the present case are desired at room temperatures for various energy applications. The manifestation of nontrivial TS governed by the unconventional band inversion mechanism and the TE properties of AuI make it a unique multi-functional candidate with probable thermoelectric and spintronic applications.
ISSN:0953-8984
1361-648X
DOI:10.1088/1361-648X/abdce8