<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Cai J</submitter><funding>Gordon and Betty Moore Foundation (Gordon E. and Betty I. Moore Foundation)</funding><funding>NSF | Directorate for Mathematical &amp; Physical Sciences | Division of Materials Research (DMR)</funding><funding>NSF | Directorate for Mathematical &amp;amp; Physical Sciences | Division of Materials Research</funding><funding>UW | Clean Energy Institute</funding><funding>Hellman Foundation</funding><funding>DOE | SC | Basic Energy Sciences (BES)</funding><funding>United States Department of Defense | United States Air Force | AFMC | Air Force Office of Scientific Research</funding><funding>Gordon and Betty Moore Foundation</funding><funding>United States Department of Defense | United States Air Force | AFMC | Air Force Office of Scientific Research (AF Office of Scientific Research)</funding><funding>DOE | SC | Basic Energy Sciences</funding><pagination>1668</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC8964814</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>13(1)</volume><pubmed_abstract>The interplay between band topology and magnetism can give rise to exotic states of matter. For example, magnetically doped topological insulators can realize a Chern insulator that exhibits quantized Hall resistance at zero magnetic field. While prior works have focused on ferromagnetic systems, little is known about band topology and its manipulation in antiferromagnets. Here, we report that MnBi&lt;sub>2&lt;/sub>Te&lt;sub>4&lt;/sub> is a rare platform for realizing a canted-antiferromagnetic (cAFM) Chern insulator with electrical control. We show that the Chern insulator state with Chern number C = 1 appears as the AFM to canted-AFM phase transition happens. The Chern insulator state is further confirmed by observing the unusual transition of the C = 1 state in the cAFM phase to the C = 2 orbital q</pubmed_abstract><journal>Nature communications</journal><pubmed_title>Electric control of a canted-antiferromagnetic Chern insulator.</pubmed_title><pmcid>PMC8964814</pmcid><funding_grant_id>GBMF9063</funding_grant_id><funding_grant_id>DMR-1719797</funding_grant_id><funding_grant_id>DE-SC0019443</funding_grant_id><funding_grant_id>DMR-2004701</funding_grant_id><funding_grant_id>FA9550-21-1-0177</funding_grant_id><pubmed_authors>Yan J</pubmed_authors><pubmed_authors>Wang C</pubmed_authors><pubmed_authors>Cai J</pubmed_authors><pubmed_authors>He M</pubmed_authors><pubmed_authors>Lin Z</pubmed_authors><pubmed_authors>Fei Z</pubmed_authors><pubmed_authors>Chu JH</pubmed_authors><pubmed_authors>Cui YT</pubmed_authors><pubmed_authors>Cobden D</pubmed_authors><pubmed_authors>Ovchinnikov D</pubmed_authors><pubmed_authors>Song T</pubmed_authors><pubmed_authors>Chang CZ</pubmed_authors><pubmed_authors>Xiao D</pubmed_authors><pubmed_authors>Xu X</pubmed_authors></additional><is_claimable>false</is_claimable><name>Electric control of a canted-antiferromagnetic Chern insulator.</name><description>The interplay between band topology and magnetism can give rise to exotic states of matter. For example, magnetically doped topological insulators can realize a Chern insulator that exhibits quantized Hall resistance at zero magnetic field. While prior works have focused on ferromagnetic systems, little is known about band topology and its manipulation in antiferromagnets. Here, we report that MnBi&lt;sub>2&lt;/sub>Te&lt;sub>4&lt;/sub> is a rare platform for realizing a canted-antiferromagnetic (cAFM) Chern insulator with electrical control. We show that the Chern insulator state with Chern number C = 1 appears as the AFM to canted-AFM phase transition happens. The Chern insulator state is further confirmed by observing the unusual transition of the C = 1 state in the cAFM phase to the C = 2 orbital q</description><dates><release>2022-01-01T00:00:00Z</release><publication>2022 Mar</publication><modification>2025-04-25T18:03:27.956Z</modification><creation>2025-04-25T18:03:27.956Z</creation></dates><accession>S-EPMC8964814</accession><cross_references><pubmed>35351900</pubmed><doi>10.1038/s41467-022-29259-8</doi></cross_references></HashMap>