{"id":38,"date":"2025-06-25T22:03:46","date_gmt":"2025-06-25T14:03:46","guid":{"rendered":"http:\/\/111.186.56.76\/?page_id=38"},"modified":"2026-05-18T21:29:36","modified_gmt":"2026-05-18T13:29:36","slug":"research","status":"publish","type":"page","link":"https:\/\/2d.sjtu.edu.cn\/index.php\/research\/","title":{"rendered":"Research"},"content":{"rendered":"\n<div class=\"wp-block-columns has-small-font-size is-layout-flex wp-container-core-columns-is-layout-3c1ab255 wp-block-columns-is-layout-flex\" style=\"margin-top:var(--wp--preset--spacing--80);margin-bottom:var(--wp--preset--spacing--80);padding-right:0;padding-left:0\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:100%\">\n<figure class=\"wp-block-gallery has-nested-images columns-default is-cropped wp-block-gallery-1 is-layout-flex wp-block-gallery-is-layout-flex\">\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"599\" data-id=\"176\" src=\"https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/transport-graphene-1024x599.png\" alt=\"\" class=\"wp-image-176\" srcset=\"https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/transport-graphene-1024x599.png 1024w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/transport-graphene-300x176.png 300w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/transport-graphene-768x449.png 768w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/transport-graphene.png 1200w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n<\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:100%\">\n<p class=\"has-heading-color has-text-color has-link-color has-large-font-size wp-elements-947760e7a22c58940395e302d7bb9b0d wp-block-paragraph\"><strong>Topological transport in 2D materials<\/strong><\/p>\n\n\n\n<p class=\"has-text-align-left has-heading-color has-text-color has-link-color has-medium-font-size wp-elements-13c4dc7670f36dac464de20770d2241f wp-block-paragraph\" style=\"margin-right:0;margin-left:0\">Topological states of quantum materials offer an exciting platform to test some profound ideas in mathematics and physics. In 2D materials we achieved to observed topological phases by electrical transport measurement. The first example is a topological valley current in bilayer graphene when the inversion symmetry is broken by an electric field.[1] A second example is topological high order Chern insulator and ferromagnetism in ABC-stacked trilayer graphene on hBN moir\u00e9 superlattice. By using a electric field, we achieve to tune the topology of the correlated flat band in the moir\u00e9 superlattice, A high order Chern insulator is observed from the quantized anomalous Hall effect.[2][3]<\/p>\n\n\n\n<p class=\"has-text-align-left has-heading-color has-text-color has-link-color has-medium-font-size wp-elements-6a4ea7e78d2cfd40982eed7cb76b12fe wp-block-paragraph\">1. Nature Physics 11 (12),1027-1031.(2015)<\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color has-medium-font-size wp-elements-ca3a2fdeb30b00cf6e70d28870af5be6 wp-block-paragraph\">2. Nature, 579,56-61.(2020)<\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color has-medium-font-size wp-elements-c5af8332ad77fb71b46650ed8e6cd997 wp-block-paragraph\">3. Physical Review Letters, 122,016401.(2019)<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-76df5cff wp-block-columns-is-layout-flex\" style=\"margin-top:var(--wp--preset--spacing--80);margin-bottom:var(--wp--preset--spacing--80)\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-gallery aligncenter has-nested-images columns-default is-cropped wp-block-gallery-2 is-layout-flex wp-block-gallery-is-layout-flex\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"1100\" height=\"823\" data-id=\"178\" src=\"https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/tunable-insulator.jpg\" alt=\"\" class=\"wp-image-178\" srcset=\"https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/tunable-insulator.jpg 1100w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/tunable-insulator-300x224.jpg 300w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/tunable-insulator-1024x766.jpg 1024w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/tunable-insulator-768x575.jpg 768w\" sizes=\"auto, (max-width: 1100px) 100vw, 1100px\" \/><\/figure>\n<\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<p class=\"has-heading-color has-text-color has-link-color has-large-font-size wp-elements-fb3514f4f0fd5d3e54eb2a2456644342 wp-block-paragraph\"><strong>Tunable correlated states and superconductivity in graphene<\/strong><\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-83784ccb41562e560aa3e76491692f7a wp-block-paragraph\">Tunable Mott insulator and superconductivity in ABC-stacked trilayer graphene on hBN moir\u00e9 superlattice. For the first time, we<br>experimentally create an ABC-stacked trilayer graphene on hBN<br>moir\u00e9 superlattice, and acheive the moir\u00e9 flat band. The<br>bandwidth and correlated strength can be conviniently tuned by<br>the vertical electric field in this system.In the strong correlated<br>regime, we observe the Mott insulating states[4] and signatures of<br>superconductivity[5].<\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-7426c013557aed8c0b2888997aa9efa1 wp-block-paragraph\">4. Nature Physics, 15, 237-241.(2019)<\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-ad64bb96e4aaa4839d16775be57b7dc8 wp-block-paragraph\">5. Nature, 572, 215-219. (2019)<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-01031cc7 wp-block-columns-is-layout-flex\" style=\"margin-top:var(--wp--preset--spacing--80);margin-bottom:var(--wp--preset--spacing--80);padding-right:0;padding-left:0\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-gallery has-nested-images columns-default is-cropped wp-block-gallery-3 is-layout-flex wp-block-gallery-is-layout-flex\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"881\" height=\"743\" data-id=\"179\" src=\"https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/electronic-property.jpg\" alt=\"\" class=\"wp-image-179\" srcset=\"https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/electronic-property.jpg 881w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/electronic-property-300x253.jpg 300w, https:\/\/2d.sjtu.edu.cn\/wp-content\/uploads\/2026\/05\/electronic-property-768x648.jpg 768w\" sizes=\"auto, (max-width: 881px) 100vw, 881px\" \/><\/figure>\n<\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<p class=\"has-heading-color has-text-color has-link-color has-large-font-size wp-elements-21a780980b110512f4bd46b0954a32b0 wp-block-paragraph\"><strong>Engineering graphene&#8217;s electronic properties by moir\u00e9 superlattice<\/strong><\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-69dcca517ee6e6bca5c5f8e7e646e6b3 wp-block-paragraph\">Graphene and hBN are both honeycomb lattices with tiny lattice constant mismatch. A long-periodic moir\u00e9 pattern forms when graphene is put on hBN with a small twisted angle. The moir\u00e9 pattern can dramatically modify the electronic properties of graphene, such as a band gap opening, secondary and tertary. Dirac points from band folding, and Hofstadter butterfly physics. <\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-2a9493c18b3cdefa0786268fd35bb061 wp-block-paragraph\">6. Nano Letters,17, 3576-3581. (2017) <\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-47663a8e2fa14677192b19168e09d232 wp-block-paragraph\">7. Nature Materials, 12, 792-797. (2013)<\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-155d0ec509d809d8809702a550822833 wp-block-paragraph\">8. Nature Physics, 12, 1111-1115. (2016)<\/p>\n\n\n\n<p class=\"has-heading-color has-text-color has-link-color wp-elements-7d9a579026fe1e018a16effe2ed4b560 wp-block-paragraph\">9. Physical Review Letters, 116 (12), 126101. (2016)<br><br>10. Nano Letters,16 (4), 2387-2392. (2016)<\/p>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Topological transport in 2D materials Topological state [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-38","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/pages\/38","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/comments?post=38"}],"version-history":[{"count":3,"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/pages\/38\/revisions"}],"predecessor-version":[{"id":199,"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/pages\/38\/revisions\/199"}],"wp:attachment":[{"href":"https:\/\/2d.sjtu.edu.cn\/index.php\/wp-json\/wp\/v2\/media?parent=38"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}