Emergence of topological semimetals in gap closing in semiconductors without inversion symmetry
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Closing of a band gap of inversion-asymmetric semiconductors always leads either to a Weyl semimetal or to a nodal-line semimetal
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The band closing transition of a semiconductor lacking inversion symmetry always proceeds through a gapless phase, consisting either of Weyl points or nodal lines.
“It has been recently argued that the band closing transition of a semiconductor lacking inversion symmetry always proceeds through a gapless phase, consisting either of Weyl points or nodal lines (Murakami et al. , 2017).”
From Weyl and Dirac semimetals in three-dimensional solids (2018) · cites this paper as Murakami et al. , 2017
The Introduction states that gap closing leads to either a Weyl semimetal or a nodal-line semimetal, and the Results reach the same conclusion for inversion-asymmetric insulators with time-reversal symmetry. The claim omits the paper’s stated restriction to three-dimensional, spinful, time-reversal-symmetric systems with nonzero spin-orbit coupling, so its unqualified “always” is broader than the result. (LLM, conf=0.88)
Experimental — accuracy not yet measuredThe symmetry of the space group and the wavevector where the gap closes uniquely determine whether the material becomes a Weyl semimetal or a nodal-line semimetal.
“The symmetry of the space group and the wavevector where the gap closes uniquely determine which possibility occurs (Murakami et al. , 2017).”
From Weyl and Dirac semimetals in three-dimensional solids (2018) · cites this paper as Murakami et al., 2017
The Results (‘One hundred thirty-eight inversion-asymmetric space groups’; page not provided) identify Weyl and nodal-line semimetals as outcomes of gap closing in inversion-asymmetric insulators with time-reversal symmetry. But the Results (‘Various cases of gap-closing events classified by symmetry’; page not provided) show that at a mirror-symmetric wavevector, the outcome also depends on the valence and conduction bands’ representations: matching mirror eigenvalues produce Weyl nodes, while different eigenvalues produce a nodal line. Space-group symmetry and wavevector alone therefore do not uniquely determine which occurs. (LLM, conf=0.88)
Experimental — accuracy not yet measuredA particularly straightforward mechanism for creation of a WSM phase occurs generically in the band inversion transition between a trivial and topological insulator if the material's space group breaks inversion symmetry.
“As discussed above, a particularly straightforward mechanism for creation of a WSM phase occurs generically in the band inversion transition between a trivial and topological insulator if the material's space group breaks inversion symmetry (Murakami, 2007; Murakami et al. , 2017).”
From Weyl and Dirac semimetals in three-dimensional solids (2018) · cites this paper as Murakami et al., 2017
On approach to the band gap inversion transition, the material becomes either a Weyl semimetal or a nodal-line semimetal for an extended region of parameter space, but there is no direct transition between the two insulating states.
“On the approach to the band gap inversion transition, the material becomes either a (i) Weyl semimetal or a (ii) nodal-line semimetal for an extended region of parameter space, but there is no direct transition between the two insulating states.”
From Weyl and Dirac semimetals in three-dimensional solids (2018) · cites this paper as Murakami et al., 2017
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Sorted by citations
Weyl and Dirac semimetals in three-dimensional solids
Armitage, N. P., Mele, E. J., & Vishwanath, A. (2018) · Reviews of Modern Physics · doi:10.1103/revmodphys.90.015001 · Cited by 4,528 · see citing works
“It has been recently argued that the band closing transition of a semiconductor lacking inversion symmetry always proceeds through a gapless phase, consisting either of Weyl points or nodal lines (Murakami et al., 2017).”
BackgroundWeyl and Dirac Semimetals in Three Dimensional Solids
Armitage, N. P., Mele, E. J., & Vishwanath, A. (2017) · arXiv
“It has been recently argued that the band closing transition of a semiconductor lacking inversion symmetry always proceeds through a gapless phase, consisting either of Weyl points or nodal lines (Murakami et al., 2017).”
Background
- Authors
- Murakami, S., Hirayama, M., Okugawa, R., & Miyake, T.
- Affiliations
- Tokyo Institute of Technology (JP)
- National Institute of Advanced Industrial Science and Technology (JP)
- Corresponding author
- Murakami, Shuichi
- Venue
- Science Advances
- Published
- 2017-05-05
- Volume
- 3
- Issue
- 5
- Pages
- e1602680-e1602680
- ISSN
- 2375-2548 (ISSN-L)
- PMC
- PMC5429037
- OpenAlex
- W2539769698
- Cited by
- 84
- References
- 8
- Citations by year
- 2026: 2 · 2025: 7 · 2024: 7 · 2023: 9 · 2022: 14 · 2021: 8 · 2020: 7 · 2019: 10 · 2018: 14 · 2017: 6
- FWCI
- 4.96
- Type
- journal article
- Language
- en
- Open access
- gold
- doi.org
- Licence
- cc-by-nc
- Locations
- Science Advances (publishedVersion, cc-by-nc)
- PubMed Central (publishedVersion, cc-by-nc)
- PubMed (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- Tokyo Tech Research Repository (Tokyo Institute of Technology) (submittedVersion)
- arXiv (Cornell University)
- Bulletin of the American Physical Society
- Funders
- Ministry of Education, Culture, Sports, Science, and Technology (ID0EM2AG17232, 26287062, ID0E5BBG17233, 26103006, ID0ESIBG17234, 16J08552, ID0ERMBG17235, Elements Strategy Initiative to Form Core Research Center (TIES))
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Topological Materials and Phenomena
- Physical Sciences › Physics and Astronomy › Condensed Matter Physics › Advanced Condensed Matter Physics
- Physical Sciences › Materials Science › Materials Chemistry › 2D Materials and Applications
- Keywords
- topological semimetals, band gap closing, Weyl semimetals, nodal-line semimetals, time-reversal symmetry, space groups, band inversion, topological phase transition
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