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Topological insulators on the square–hexagon lattice driven by next-nearest-neighbor hopping
We investigate the topological phase transition of the square-hexagon lattice driven by the next-nearest-neighbor (NNN) hopping. By means of the Fukui-Hatsugai method, the topological invariant can be determined. The phase diagrams in the ( , ) plane for different filling fractions are displayed, to...
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Published in: | Journal of physics. Condensed matter 2022-07, Vol.34 (27), p.275501 |
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creator | Wang, Guo Xiang Zhang, Ying Zheng Wei, Jun Hong |
description | We investigate the topological phase transition of the square-hexagon lattice driven by the next-nearest-neighbor (NNN) hopping. By means of the Fukui-Hatsugai method, the topological invariant
can be determined. The phase diagrams in the (
,
) plane for different filling fractions are displayed, together with the size of the bulk band gap. We find the competition between
and
can drive the system into topological nontrivial phase, with
= 1. Interestingly, for 2/5 and 3/5 filling fractions, topological nontrivial phase can be easily realized when the NNN hoppings are turned on. Besides, the phase diagrams in the plane of
and
(
and
) are also investigated. By numerically diagonalizing the Hamiltonian, the bulk band structures are calculated. And the topological trivial and nontrivial phase are also distinguished in terms of helical edge state. In experiments, these topological phase transitions may be realized by shaking optical lattice. |
doi_str_mv | 10.1088/1361-648X/ac6788 |
format | article |
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can be determined. The phase diagrams in the (
,
) plane for different filling fractions are displayed, together with the size of the bulk band gap. We find the competition between
and
can drive the system into topological nontrivial phase, with
= 1. Interestingly, for 2/5 and 3/5 filling fractions, topological nontrivial phase can be easily realized when the NNN hoppings are turned on. Besides, the phase diagrams in the plane of
and
(
and
) are also investigated. By numerically diagonalizing the Hamiltonian, the bulk band structures are calculated. And the topological trivial and nontrivial phase are also distinguished in terms of helical edge state. In experiments, these topological phase transitions may be realized by shaking optical lattice.</description><identifier>ISSN: 0953-8984</identifier><identifier>EISSN: 1361-648X</identifier><identifier>DOI: 10.1088/1361-648X/ac6788</identifier><identifier>PMID: 35421856</identifier><identifier>CODEN: JCOMEL</identifier><language>eng</language><publisher>England: IOP Publishing</publisher><subject>square–hexagon lattice ; tight-binding model ; topological phase transition</subject><ispartof>Journal of physics. Condensed matter, 2022-07, Vol.34 (27), p.275501</ispartof><rights>2022 IOP Publishing Ltd</rights><rights>2022 IOP Publishing Ltd.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c368t-264bf4a48debcc18725652dc2c5735830468b0767c73a08a34abb27085ba6743</citedby><cites>FETCH-LOGICAL-c368t-264bf4a48debcc18725652dc2c5735830468b0767c73a08a34abb27085ba6743</cites><orcidid>0000-0002-2353-9629</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/35421856$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Wang, Guo Xiang</creatorcontrib><creatorcontrib>Zhang, Ying Zheng</creatorcontrib><creatorcontrib>Wei, Jun Hong</creatorcontrib><title>Topological insulators on the square–hexagon lattice driven by next-nearest-neighbor hopping</title><title>Journal of physics. Condensed matter</title><addtitle>JPhysCM</addtitle><addtitle>J. Phys.: Condens. Matter</addtitle><description>We investigate the topological phase transition of the square-hexagon lattice driven by the next-nearest-neighbor (NNN) hopping. By means of the Fukui-Hatsugai method, the topological invariant
can be determined. The phase diagrams in the (
,
) plane for different filling fractions are displayed, together with the size of the bulk band gap. We find the competition between
and
can drive the system into topological nontrivial phase, with
= 1. Interestingly, for 2/5 and 3/5 filling fractions, topological nontrivial phase can be easily realized when the NNN hoppings are turned on. Besides, the phase diagrams in the plane of
and
(
and
) are also investigated. By numerically diagonalizing the Hamiltonian, the bulk band structures are calculated. And the topological trivial and nontrivial phase are also distinguished in terms of helical edge state. In experiments, these topological phase transitions may be realized by shaking optical lattice.</description><subject>square–hexagon lattice</subject><subject>tight-binding model</subject><subject>topological phase transition</subject><issn>0953-8984</issn><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp9kMtKAzEUhoMoWqt7VzI7XTiae9KlFG8guOnClSHJpG3KdDJNZkR3voNv6JOY0upKhAMHzvnOT_IBcILgJYJSXiHCUcmpfL7Slgspd8Dgd7QLBnDESClHkh6Aw5QWEEIqCd0HB4RRjCTjA_AyCW2ow8xbXRe-SX2tuxBTEZqim7sirXod3dfH59y96Vke5nXnrSuq6F9dU5j3onFvXdm4jKV197O5CbGYh7b1zewI7E11ndzxtg_B5PZmMr4vH5_uHsbXj6UlXHYl5tRMqaaycsZaJAVmnOHKYssEYZJAyqWBggsriIZSE6qNwQJKZjQXlAzB-Sa2jWHV54eopU_W1bVuXOiTwpwhPsJIoIzCDWpjSCm6qWqjX-r4rhBUa6lqbVCtDaqN1Hxyuk3vzdJVvwc_FjNwsQF8aNUi9LHJf_0v7-wP3C4VoQqLXIxBpNpqSr4BJ6yPTg</recordid><startdate>20220706</startdate><enddate>20220706</enddate><creator>Wang, Guo Xiang</creator><creator>Zhang, Ying Zheng</creator><creator>Wei, Jun Hong</creator><general>IOP Publishing</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0002-2353-9629</orcidid></search><sort><creationdate>20220706</creationdate><title>Topological insulators on the square–hexagon lattice driven by next-nearest-neighbor hopping</title><author>Wang, Guo Xiang ; Zhang, Ying Zheng ; Wei, Jun Hong</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c368t-264bf4a48debcc18725652dc2c5735830468b0767c73a08a34abb27085ba6743</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>square–hexagon lattice</topic><topic>tight-binding model</topic><topic>topological phase transition</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wang, Guo Xiang</creatorcontrib><creatorcontrib>Zhang, Ying Zheng</creatorcontrib><creatorcontrib>Wei, Jun Hong</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wang, Guo Xiang</au><au>Zhang, Ying Zheng</au><au>Wei, Jun Hong</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Topological insulators on the square–hexagon lattice driven by next-nearest-neighbor hopping</atitle><jtitle>Journal of physics. Condensed matter</jtitle><stitle>JPhysCM</stitle><addtitle>J. Phys.: Condens. Matter</addtitle><date>2022-07-06</date><risdate>2022</risdate><volume>34</volume><issue>27</issue><spage>275501</spage><pages>275501-</pages><issn>0953-8984</issn><eissn>1361-648X</eissn><coden>JCOMEL</coden><abstract>We investigate the topological phase transition of the square-hexagon lattice driven by the next-nearest-neighbor (NNN) hopping. By means of the Fukui-Hatsugai method, the topological invariant
can be determined. The phase diagrams in the (
,
) plane for different filling fractions are displayed, together with the size of the bulk band gap. We find the competition between
and
can drive the system into topological nontrivial phase, with
= 1. Interestingly, for 2/5 and 3/5 filling fractions, topological nontrivial phase can be easily realized when the NNN hoppings are turned on. Besides, the phase diagrams in the plane of
and
(
and
) are also investigated. By numerically diagonalizing the Hamiltonian, the bulk band structures are calculated. And the topological trivial and nontrivial phase are also distinguished in terms of helical edge state. In experiments, these topological phase transitions may be realized by shaking optical lattice.</abstract><cop>England</cop><pub>IOP Publishing</pub><pmid>35421856</pmid><doi>10.1088/1361-648X/ac6788</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0002-2353-9629</orcidid></addata></record> |
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source | Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List) |
subjects | square–hexagon lattice tight-binding model topological phase transition |
title | Topological insulators on the square–hexagon lattice driven by next-nearest-neighbor hopping |
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