Controllable topological phase transition <i>via</i> ferroelectric–paraelectric switching in a ferromagnetic single-layer M<sub>I</sub>M<sub>II</sub>Ge<sub>2</sub>X<sub>6</sub> family

Recently, the emergence of two-dimensional (2D) multiferroic materials has opened a new perspective for exploring topological states. However, instances of tuning topological phase transitions through ferroelectric (FE) polarization in 2D ferromagnetic (FM) materials are relatively rare. Here, we found that 11 single layer (SL) materials, named the M<sub>I</sub>M<sub>II</sub>Ge<sub>2</sub>X<sub>6</sub> family, possess both FE and FM properties. Among them, 5 SL materials exhibit controllable topological phase transition <i>via</i> ferroelectric-paraelectric switching. Taking the SL ReIrGe<sub>2</sub>S<sub>6</sub> as an example, we find that the paraelectric (PE) and FE phases exhibit half-metal and magnetic semiconductor behavior, respectively. In the spin-down channel of the PE phase, a critical-type Weyl point (WP) is observed with a robust Fermi arc edge state. In contrast, the FE phase of the SL ReIrGe<sub>2</sub>S<sub>6</sub> clearly identifies 0D corner states in both spin channels. Therefore, under the control of external fields, the SL ReIrGe<sub>2</sub>S<sub>6</sub> undergoes a transformation from PE to FE by overcoming the energy barrier of 0.62 eV, subsequently realizing the phase transition from the Weyl semimetal to the high order topological insulator. These findings not only combine topological states with multiferroics but also pave the way for the experimental discovery of 2D tunable topological phase transition.

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Publication Details

Journal
Materials Horizons
Published
2024-12-24
DOI
https://doi.org/10.1039/d4mh01599a
Citations
5
Primary Topic
Solid-state spectroscopy and crystallography
Type
article
Field-Weighted Citation Impact
0.59

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Controllable topological phase transition via ferroelectric–paraelectric switching in a ferromagnetic single-layer MIMIIGe2X6 family

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Materials Horizons
Solid-state spectroscopy and crystallography
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article

Controllable topological phase transition via ferroelectric–paraelectric switching in a ferromagnetic single-layer MIMIIGe2X6 family

Tie Yang, Zhenxiang Cheng, Jingbo Bai, Zhenzhou Guo, Weizhen Meng, Yalong Jiao, Ying Liu
article en
5 citations

Abstract

Recently, the emergence of two-dimensional (2D) multiferroic materials has opened a new perspective for exploring topological states. However, instances of tuning topological phase transitions through ferroelectric (FE) polarization in 2D ferromagnetic (FM) materials are relatively rare. Here, we found that 11 single layer (SL) materials, named the M<sub>I</sub>M<sub>II</sub>Ge<sub>2</sub>X<sub>6</sub> family, possess both FE and FM properties. Among them, 5 SL materials exhibit controllable topological phase transition <i>via</i> ferroelectric-paraelectric switching. Taking the SL ReIrGe<sub>2</sub>S<sub>6</sub> as an example, we find that the paraelectric (PE) and FE phases exhibit half-metal and magnetic semiconductor behavior, respectively. In the spin-down channel of the PE phase, a critical-type Weyl point (WP) is observed with a robust Fermi arc edge state. In contrast, the FE phase of the SL ReIrGe<sub>2</sub>S<sub>6</sub> clearly identifies 0D corner states in both spin channels. Therefore, under the control of external fields, the SL ReIrGe<sub>2</sub>S<sub>6</sub> undergoes a transformation from PE to FE by overcoming the energy barrier of 0.62 eV, subsequently realizing the phase transition from the Weyl semimetal to the high order topological insulator. These findings not only combine topological states with multiferroics but also pave the way for the experimental discovery of 2D tunable topological phase transition.

Materials HorizonsVol. 12(7)
Southwest University (CN), University of Wollongong (AU), Hebei Normal University (CN)
National Natural Science Foundation of China, Hebei Normal University, Natural Science Foundation of Hebei Province
Openalex Percentile: Top 32%
Solid-state spectroscopy and crystallography
0.59
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