Topological order and absence of band insulators at integer filling in non-symmorphic crystals
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This presents an example of a 'filling enforced semimetal' where the zone boundary degeneracy requires that electron count for a filled band actually results in a gapless state where the conduction and valence bands contact each other.
“This presents an example of a 'filling enforced semimetal' (Parameswaran, 2015; Parameswaran et al. , 2013; Watanabe et al. , 2015) where the zone boundary degeneracy requires that electron count for a filled band actually results in a gapless state where the conduction and valence bands contact each other.”
From Weyl and Dirac semimetals in three-dimensional solids (2018) · cites this paper as Parameswaran et al., 2013
The Band Theory discussion (p. 2) says that non-symmorphic symmetry prevents fewer than S bands from separating and gives an hcp example with enforced band contacts. Figure 2’s caption (p. 4) says those contacts require a minimum filling of S = 2 for a band insulator. Our copy does not specify that the contacts occur at the zone boundary, so it does not establish that part of the claim. (LLM, conf=0.83)
Experimental — accuracy not yet measuredScrew symmetries lead to double degeneracy for all Bloch states on certain planes in the Brillouin zone.
“It is known that screw symmetries lead to double degeneracy for all Bloch states on certain planes in the Brillouin zone (BZ).36,37”
From Type-II Dirac photons (2017) · cites this paper as [37]
The Band Theory section (p. 2) says nonsymmorphic symmetry prevents certain bands from being separated, and Fig. 2 (p. 4) shows screw-symmetry-enforced contacts between pairs of bands. The copy does not say that every Bloch state is doubly degenerate across particular Brillouin-zone planes; its discussion of invariant planes in the Fourier-Space Approach (p. 7) concerns a many-body degeneracy argument, not that claim. (LLM, conf=0.86)
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“This presents an example of a “filling enforced semimetal” (Parameswaran, 2015; Parameswaran et al., 2013; Watanabe et al., 2015) where the zone boundary degeneracy requires that electron count for a filled band actually results in a gapless state where the conduction and valence bands contact each…”
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- Authors
- Parameswaran, S. A., Turner, A. M., Arovas, D. P., & Vishwanath, A.
- Affiliations
- University of California, Berkeley (US)
- Institute for Theoretical Physics Amsterdam (NL)
- University of California San Diego (US)
- Lawrence Berkeley National Laboratory (US)
- Corresponding author
- Vishwanath, Ashvin
- Venue
- Nature Physics
- Published
- 2013-04-14
- Volume
- 9
- Issue
- 5
- Pages
- 299-303
- ISSN
- 1745-2473 (ISSN-L)
- 1745-2481
- OpenAlex
- W1975117261
- Cited by
- 184
- References
- 40
- Citations by year
- 2026: 1 · 2025: 4 · 2024: 19 · 2023: 9 · 2022: 9 · 2021: 18 · 2020: 17 · 2019: 16 · 2018: 20 · 2017: 27 · 2016: 27 · 2015: 12 · 2014: 3 · 2013: 2
- FWCI
- 7.55
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Licence
- www.springer.com/tdm (tdm)
- Locations
- Nature Physics (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- arXiv (Cornell University)
- 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 › Physics and Astronomy › Condensed Matter Physics › Physics of Superconductivity and Magnetism
- Keywords
- topological order, band insulator, integer filling, Mott insulator, lattice symmetry, gapped ground states, quantum spin systems, fractionalized excitations, three-dimensional crystals
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