# A first-principles investigation of Topological Phase Transition in   face-centred cubic LiMgBi

**Authors:** Raghottam M Sattigeri, Sharad Babu Pillai, Prafulla K Jha, Brahmananda, Chakraborty

arXiv: 1905.10103 · 2019-08-23

## TL;DR

This study uses first-principles calculations to reveal a topological phase transition in LiMgBi under volume expansion, transforming it from a band insulator to a strong topological insulator with potential applications in electronics and spintronics.

## Contribution

It is the first to identify and characterize a topological phase transition in face-centered cubic LiMgBi driven by volume expansion using first-principles methods.

## Key findings

- LiMgBi undergoes a topological phase transition at 4.0% volume expansion.
- The phase transition results in a Dirac semi-metal with band inversion.
- LiMgBi is identified as a strong topological insulator with potential applications.

## Abstract

Topological Insulators (TI) exhibit robust spin-locked dissipationless Fermion transport along the surface states. In the current study, we use \textit{first-principles} calculations to investigate a Topological Phase Transition (TPT) in a Half-Heusler (HH) compound LiMgBi driven by a Volume Expansive Pressure (VEP) which is attributed to the presence of, intrinsic voids, thermal perturbations and/or due to a phenomena known as cavity nuclei. We find that, the dynamically stable \textit{face-centred cubic} (FCC) structure of LiMgBi (which belongs to the F$\overline{4}$3m[216] space group), undergoes TPT beyond a critical VEP at 4.0\%. The continuous application of VEP from 0.0\% to 8.0\% results in a phase transition from a, band insulator to a Dirac semi-metal nature. Qualitatively, the Dirac cone formation and band inversion along the high symmetry point $\mathbf{\Gamma}$ in the Brillouin Zone (BZ) are analysed in terms of Electronic Band Structure (EBS) and Projected Local Density of States (LDOS). The TPT is further characterised by the $\mathbb{Z}_2$ invariant, ($\nu_0$, $\nu_1$ $\nu_2$ $\nu_3$) $\equiv$ (1, 0 0 0) along the (0001) surface which indicates quantitatively that, HH LiMgBi is a strong TI. We hence propose, HH LiMgBi (known for its piezoelectric, thermo-electric and semi-conducting applications) as a strong TI with potential multipurpose application in the field of electronics, spintronics and quantum computation.

## Full text

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## Figures

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## References

57 references — full list in the complete paper: https://tomesphere.com/paper/1905.10103/full.md

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Source: https://tomesphere.com/paper/1905.10103