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Line-Node Dirac Semimetal and Topological Insulating Phase in Noncentrosymmetric Pnictides CaAgX (X = P, As)

Published 1 Oct 2015 in cond-mat.mes-hall | (1510.00202v3)

Abstract: Two noncentrosymmetric ternary pnictides, CaAgP and CaAgAs, are reported as topological line-node semimetals protected solely by mirror-reflection symmetry. The band gap vanishes on a circle in momentum space, and surface states emerge within the circle. Extending this study to spin-orbit coupled systems reveals that, compared with CaAgP, a substantial band gap is induced in CaAgAs by large spin-orbit interaction. The resulting states are a topological insulator, in which the Z2 topological invariant is given by 1; 000. To clarify the Z2 topological invariants for time-reversal-invariant systems without spatial-inversion symmetry, we introduce an alternative way to calculate the invariants characterizing a line node and topological insulator for mirror-reflection-invariant systems.

Citations (164)

Summary

Line-Node Dirac Semimetal and Topological Insulating Phase in Noncentrosymmetric Pnictides CaAgX (X= P, As)

The paper under consideration investigates the electronic properties of noncentrosymmetric pnictides, focusing on CaAgP and CaAgAs, as potential candidates for line-node Dirac semimetals and topological insulators. The primary objective of this research is to explore the novel line-node semimetallic state in CaAgX compounds and their transition to topological insulating phases upon the inclusion of spin-orbit interaction (SOI).

Key Findings and Methodology

The authors employ first-principles calculations, supplemented by tight-binding models, to analyze the electronic band structure of CaAgP and CaAgAs compounds. These investigations reveal that:

  1. Line-Node Dirac Semimetal State: CaAgP and CaAgAs lack spatial inversion symmetry yet can host line nodes due to the presence of mirror-reflection symmetry. In the absence of SOI, CaAgP exhibits a line-node Dirac semimetal state where the band gap vanishes along a closed loop in momentum space. This feature is critically dependent on the mirror symmetry, which ensures the degeneracy of energy bands on invariant planes.
  2. Influence of Spin-Orbit Interaction: The inclusion of SOI profoundly impacts the electronic properties. In CaAgP, due to weak spin-orbit coupling in phosphorus, the line node is only slightly gapped, maintaining the semimetallic characteristics. On the contrary, CaAgAs exhibits a substantial band gap due to the stronger spin-orbit coupling in arsenic, leading to a topological insulating state characterized by a Z2\mathbb Z_2 invariant of $1;000$.
  3. Topological Phases and Surface States: The paper introduces an alternative method for calculating Z2\mathbb Z_2 topological invariants for systems lacking spatial inversion symmetry. This methodological advancement aids in assessing the topological nature of electronic states and their transitions. The surface states corroborate the bulk-boundary correspondence, exhibiting gapless states on specific surfaces, which are distinct depending on the termination layer type.

Numerical Results and Technical Insights

The numerical results reveal that in CaAgAs, SOI creates a sizable band gap of approximately 1000 K, which is an order of magnitude stronger than in CaAgP. This significant difference underscores the transition from a semimetal to a topological insulator. The work further identifies that in CaAgP, the induced gap is around 10 K due to weaker SOI, which highlights the subtle yet critical impact of atomic composition and SOI on topological phase transitions.

Implications and Future Directions

From a theoretical perspective, the findings suggest that exploring materials with noncentrosymmetric crystal structures, particularly those with pronounced mirror symmetries, is promising for discovering new topological phases. Practically, such systems could expand the repertoire of materials suitable for realizing topological quantum computing, given the robust surface states in topological insulators.

For future research, it would be pertinent to investigate the interplay of electron correlations with topological properties in these and similar materials. Moreover, exploring the effects of external parameters, such as pressure or doping, could further tune the topological characteristics, potentially uncovering new phases or enhancing the stability of existing ones.

The research contributes a nuanced understanding of topological electronic structures in the context of condensed matter physics, offering a refined approach to classify topological invariants in systems with intricate symmetries. The insights gleaned from this study could propel advancements in material science where topological properties play a pivotal role in applications like spintronics and quantum devices.

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