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Altermagnetism-induced higher-order topological Dirac semimetals in two-dimensional nonsymmorphic systems

Abstract

We propose an altermagnetism-induced route to a two-dimensional higher-order topological Dirac semimetal in a trilayer nonsymmorphic Dirac system. Interlayer hybridization preserves the nonsymmorphic bulk Dirac crossings and generates helical edge states in the trilayer phase. Introducing outer-layer d-wave altermagnetic order gaps the helical edge states, while only the symmetry-protected Dirac crossing at high-symmetry point M remains gapless. The resulting phase hosts a surviving bulk Dirac point, gapped edge spectra, and corner states. An exact layer-space decomposition further reveals that these features arise from the coexistence of a gapless Dirac sector and a gapped ℤ2 topological sector. Our results establish altermagnetism as an effective mechanism for engineering higher-order topological Dirac semimetals in two-dimensional nonsymmorphic systems.

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BibTeX
@misc{liu2026altermagnetisminduced,
  title = {{Altermagnetism-induced higher-order topological Dirac semimetals in two-dimensional nonsymmorphic systems}},
  author = {Lizhou Liu and Cheng-Ming Miao and Ying-Tao Zhang and Qing-Feng Sun},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.04347},
  eprint = {2611.04347},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.04347},
}
RIS
TY  - UNPB
TI  - Altermagnetism-induced higher-order topological Dirac semimetals in two-dimensional nonsymmorphic systems
AU  - Lizhou Liu
AU  - Cheng-Ming Miao
AU  - Ying-Tao Zhang
AU  - Qing-Feng Sun
PY  - 2026
DA  - 2026/11/03
PB  - arXiv
DO  - 10.48550/arxiv.2611.04347
UR  - https://arxiv.org/abs/2611.04347
AB  - We propose an altermagnetism-induced route to a two-dimensional higher-order topological Dirac semimetal in a trilayer nonsymmorphic Dirac system. Interlayer hybridization preserves the nonsymmorphic bulk Dirac crossings and generates helical edge states in the trilayer phase. Introducing outer-layer d-wave altermagnetic order gaps the helical edge states, while only the symmetry-protected Dirac crossing at high-symmetry point M remains gapless. The resulting phase hosts a surviving bulk Dirac point, gapped edge spectra, and corner states. An exact layer-space decomposition further reveals that these features arise from the coexistence of a gapless Dirac sector and a gapped ℤ_2 topological sector. Our results establish altermagnetism as an effective mechanism for engineering higher-order topological Dirac semimetals in two-dimensional nonsymmorphic systems.
ER  -