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Unraveling the Secrets of Dirac Semimetals

Discover the unique electronic properties of Dirac semimetals and their fascinating transitions.

― 4 min read


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Table of Contents

Dirac semimetals are a type of material that has unique electronic properties. They contain special points called Dirac Points where the conduction band and valence band meet. This crossing point behaves like a particle called a Dirac fermion, which has massless characteristics. The structure of these materials is crucial for understanding their behavior in different conditions.

Lifshitz Transition

One interesting feature of Dirac semimetals is the Lifshitz transition. This transition occurs when the shape of the material's electronic structure changes. Such changes can happen without altering the fundamental symmetry of the material. In the case of Dirac semimetals, this often involves the behavior of the Fermi Arcs, which are connected states on the surface of the material.

Role of Fermi Arcs

Fermi arcs are critical in how electrons behave on the surface of Dirac semimetals. They serve as pathways for electrons and connect different Dirac points. When these Fermi arcs change, it can lead to new electronic phenomena. The Lifshitz transition can essentially deform these arcs, causing them to either connect or disconnect from the bulk Dirac points below the surface.

Magnetotransport and Quantum Hall Effect

When a magnetic field is applied to a Dirac semimetal, it can induce effects such as the quantum Hall effect (QHE). The QHE occurs when electrons move in a circular motion due to the magnetic field, leading to quantized levels of conductivity. This means that the conductivity values become sharply defined, leading to plateaus in measurements.

Interaction of Fermi Arcs and Weyl Orbits

In Dirac semimetals, the connection between Fermi arcs and Weyl orbits is essential. Weyl orbits arise from the pairing of Dirac points, leading to a rich structure of surface and bulk states. However, when the Fermi arcs are influenced by the Lifshitz transition, it can disrupt the Weyl orbit mechanism. This is significant because it changes the way the quantum Hall effect manifests in the material.

How the Structure Affects Quantum Hall Behavior

The thickness of a Dirac semimetal can greatly influence its quantum Hall behavior. In very thin samples, the properties may differ significantly compared to thicker ones. This thickness dependence comes into play during transitions and can lead to irregularities in the quantized Hall plateaus.

Effects of Bulk Perturbations

In real materials, imperfections and variations (bulk perturbations) are unavoidable. These bulk perturbations can affect the physical properties of the semimetals, particularly the Fermi arcs and Weyl orbits. As the Lifshitz transition occurs, the presence of bulk perturbations must be considered to fully understand the electronic behavior.

Surface States and Landau Levels

The surface states of Dirac semimetals are influenced by magnetic fields. When the quantum Hall effect is activated, Landau levels (quantized energy levels) can form in response to the magnetic field. These levels are essential for the electrical properties observed in experiments. The formation of Landau levels indicates how surface and bulk states interact with each other and are crucial in understanding the material's overall behavior.

Observation and Challenges

Observing the unique features of Dirac semimetals can be challenging. Spectroscopic techniques can struggle to resolve the fine details of the electronic structure. Therefore, alternative approaches, such as transport measurements, are often employed. These techniques can provide insights by measuring how current flows through the material under various conditions.

Scientific Implications

The research on Dirac semimetals and the quantum Hall effect has broad implications. It contributes to our understanding of exotic states of matter, which can lead to new applications in electronics, quantum computing, and materials science. The interplay between structure, magnetic fields, and electronic states offers potential pathways for developing advanced technologies.

Conclusion

In summary, Dirac semimetals are fascinating materials with rich electronic behavior. The Lifshitz transition plays a significant role in how these materials function, particularly in relation to Fermi arcs and Weyl orbits. Understanding these transitions and their effects on the quantum Hall effect provides valuable insights into the behavior of electrons in these unique materials. As research continues, we can expect to uncover more about the properties and potential applications of Dirac semimetals in various fields.

Original Source

Title: Quantum Hall effect in topological Dirac semimetals modulated by the Lifshitz transition of the Fermi arc surface states

Abstract: We investigate the magnetotransport of topological Dirac semimetals (DSMs) by taking into account the Lifshitz transition of the Fermi arc surface states. We demonstrate that a bulk momentum-dependent gap term, which is usually neglected in study of the bulk energy-band topology, can cause the Lifshitz transition by developing an additional Dirac cone for the surface to prevent the Fermi arcs from connecting the bulk Dirac points. As a result, the Weyl orbits can be turned off by the surface Dirac cone without destroying the bulk Dirac points. In response to the surface Lifshitz transition, the Weyl-orbit mechanism for the 3D quantum Hall effect (QHE) in topological DSMs will break down. The resulting quantized Hall plateaus can be thickness-dependent, similar to the Weyl-orbit mechanism, but their widths and quantized values become irregular. Accordingly, we propose that apart from the bulk Weyl nodes and Fermi arcs, the surface Lifshitz transition is also crucial for realizing stable Weyl orbits and 3D QHE in real materials.

Authors: Tao-Rui Qin, Zhuo-Hua Chen, Tian-Xing Liu, Fu-Yang Chen, Hou-Jian Duan, Ming-Xun Deng, Rui-Qiang Wang

Last Update: 2023-09-15 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2309.08233

Source PDF: https://arxiv.org/pdf/2309.08233

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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