Unraveling the topological phase in Zintl semiconductors RbZn<sub>4</sub>X<sub>3</sub> (X = P, As) through band engineering

We report the topological phase transition (TPT) in compounds of relatively less explored Zintl family RbZn<sub>4</sub>X<sub>3</sub>(X = P, As) via<i>first-principles</i>calculation. These intermetallic compounds have already been experimentally synthesized in a<i>KCu<sub>4</sub>S<sub>3</sub>-type</i>tetragonal structure (P4/mmm) and reported to have a topologically trivial semimetallic nature with a direct band gap. We thoroughly studied the electronic structure, stability of RbZn<sub>4</sub>X<sub>3</sub>(X = P, As) and demonstrated the TPTs in these materials with external applied pressure and epitaxial strain. The dynamical and mechanical stabilities of these compounds are verified through phonon dispersion and Born stability criteria at ambient and TPT pressure/strain. A topologically non-trivial phase in RbZn<sub>4</sub>P<sub>3</sub>(RbZn<sub>4</sub>As<sub>3</sub>) is observed at 45 GPa (38 GPa) of hydrostatic pressure and 10% (8%) of epitaxial strain. This non-trivial phase is identified by band inversion between<i>Zn-s</i>and<i>P/As-p<sub>z</sub>orbitals</i>in the bulk band structure of these materials which is further confirmed using the surface density of states and Fermi arc contour in<i>(001)-plane</i>. The ℤ<sub>2</sub>topological invariants (<i>ν</i><sub>0</sub><i>; ν</i><sub>1</sub><i>ν</i><sub>2</sub><i>ν</i><sub>3</sub>) for these materials are calculated using the product of parities of all filled bands (Kane and Mele model) and the evolution of Wannier charge centers (Wilson loop method). The change in values of (<i>ν</i><sub>0</sub><i>; ν</i><sub>1</sub><i>ν</i><sub>2</sub><i>ν</i><sub>3</sub>) from (<i>0; 000</i>) to (<i>1; 000</i>), at the particular values of pressure and strain, is another signature of the TPT in these materials.

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Journal
Journal of Physics Condensed Matter
Published
2025-03-17
DOI
https://doi.org/10.1088/1361-648x/adc17e
Citations
4
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
Field-Weighted Citation Impact
5.03
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article

Unraveling the topological phase in Zintl semiconductors RbZn4X3 (X = P, As) through band engineering

Antik Sihi, Rajesh Kumar, Mukhtiyar Singh, Ramesh Kumar
4 citations
Journal of Physics Condensed Matter
Physics of Superconductivity and Magnetism
5.03
article

Unraveling the topological phase in Zintl semiconductors RbZn4X3 (X = P, As) through band engineering

Antik Sihi, Rajesh Kumar, Mukhtiyar Singh, Ramesh Kumar
article en
4 citations

Abstract

We report the topological phase transition (TPT) in compounds of relatively less explored Zintl family RbZn<sub>4</sub>X<sub>3</sub>(X = P, As) via<i>first-principles</i>calculation. These intermetallic compounds have already been experimentally synthesized in a<i>KCu<sub>4</sub>S<sub>3</sub>-type</i>tetragonal structure (P4/mmm) and reported to have a topologically trivial semimetallic nature with a direct band gap. We thoroughly studied the electronic structure, stability of RbZn<sub>4</sub>X<sub>3</sub>(X = P, As) and demonstrated the TPTs in these materials with external applied pressure and epitaxial strain. The dynamical and mechanical stabilities of these compounds are verified through phonon dispersion and Born stability criteria at ambient and TPT pressure/strain. A topologically non-trivial phase in RbZn<sub>4</sub>P<sub>3</sub>(RbZn<sub>4</sub>As<sub>3</sub>) is observed at 45 GPa (38 GPa) of hydrostatic pressure and 10% (8%) of epitaxial strain. This non-trivial phase is identified by band inversion between<i>Zn-s</i>and<i>P/As-p<sub>z</sub>orbitals</i>in the bulk band structure of these materials which is further confirmed using the surface density of states and Fermi arc contour in<i>(001)-plane</i>. The ℤ<sub>2</sub>topological invariants (<i>ν</i><sub>0</sub><i>; ν</i><sub>1</sub><i>ν</i><sub>2</sub><i>ν</i><sub>3</sub>) for these materials are calculated using the product of parities of all filled bands (Kane and Mele model) and the evolution of Wannier charge centers (Wilson loop method). The change in values of (<i>ν</i><sub>0</sub><i>; ν</i><sub>1</sub><i>ν</i><sub>2</sub><i>ν</i><sub>3</sub>) from (<i>0; 000</i>) to (<i>1; 000</i>), at the particular values of pressure and strain, is another signature of the TPT in these materials.

Journal of Physics Condensed MatterVol. 37(18)
West Virginia University (US), Delhi Technological University (IN)
Openalex Percentile: Top 5%
Physics of Superconductivity and Magnetism
5.03
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