Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system
Abstract We theoretically report the finding of a new kind of topological phase transition between a normal insulator and a topological metal state where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal...
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Nature Portfolio
2021
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oai:doaj.org-article:db392fe52cf0464aa7556d49ca35ad512021-12-02T16:07:02ZTopological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system10.1038/s41598-021-92390-x2045-2322https://doaj.org/article/db392fe52cf0464aa7556d49ca35ad512021-06-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-92390-xhttps://doaj.org/toc/2045-2322Abstract We theoretically report the finding of a new kind of topological phase transition between a normal insulator and a topological metal state where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal phase is characterized by stable zero-energy localized edge states that exist within the full gapless bulk states. Such states living on a quasi-one-dimensional system with three sublattices per unit cell are protected by hidden inversion symmetry. While other required symmetries such as chiral, particle-hole, or full inversion symmetry are absent in the system.Milad JangjanMir Vahid HosseiniNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-7 (2021) |
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Medicine R Science Q Milad Jangjan Mir Vahid Hosseini Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
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Abstract We theoretically report the finding of a new kind of topological phase transition between a normal insulator and a topological metal state where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal phase is characterized by stable zero-energy localized edge states that exist within the full gapless bulk states. Such states living on a quasi-one-dimensional system with three sublattices per unit cell are protected by hidden inversion symmetry. While other required symmetries such as chiral, particle-hole, or full inversion symmetry are absent in the system. |
format |
article |
author |
Milad Jangjan Mir Vahid Hosseini |
author_facet |
Milad Jangjan Mir Vahid Hosseini |
author_sort |
Milad Jangjan |
title |
Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
title_short |
Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
title_full |
Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
title_fullStr |
Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
title_full_unstemmed |
Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
title_sort |
topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system |
publisher |
Nature Portfolio |
publishDate |
2021 |
url |
https://doaj.org/article/db392fe52cf0464aa7556d49ca35ad51 |
work_keys_str_mv |
AT miladjangjan topologicalphasetransitionbetweenanormalinsulatorandatopologicalmetalstateinaquasionedimensionalsystem AT mirvahidhosseini topologicalphasetransitionbetweenanormalinsulatorandatopologicalmetalstateinaquasionedimensionalsystem |
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1718384809692102656 |