Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/113724
DC FieldValueLanguage
dc.contributorDepartment of Applied Physicsen_US
dc.creatorYan, Zen_US
dc.creatorHu, Wen_US
dc.creatorZhou, Len_US
dc.creatorHan, Xen_US
dc.creatorJiang, Jen_US
dc.creatorYin, Hen_US
dc.creatorQiu, Yen_US
dc.creatorHe, Hen_US
dc.creatorLau, SPen_US
dc.creatorWang, Gen_US
dc.date.accessioned2025-06-19T06:23:30Z-
dc.date.available2025-06-19T06:23:30Z-
dc.identifier.issn1932-7447en_US
dc.identifier.urihttp://hdl.handle.net/10397/113724-
dc.language.isoenen_US
dc.publisherAmerican Chemical Societyen_US
dc.titleTopological hall effect in Bi/Cr₂Te₃ heterostructure thin filmsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage715en_US
dc.identifier.epage721en_US
dc.identifier.volume129en_US
dc.identifier.issue1en_US
dc.identifier.doi10.1021/acs.jpcc.4c06440en_US
dcterms.abstractThe topological Hall effect (THE) due to the spatially varying magnetizations appears as humps and dips near the coercive field in the Hall resistance curves. It is possible that magnetic skyrmions might be applied to next-generation data storage devices. Previous calculations predicted that the combination of Cr2Te3 thin film with strong perpendicular anisotropy (PMA) and Bi with strong spin-orbit coupling (SOC) could induce Dzyaloshinskii-Moriya interaction (DMI) and magnetic skyrmions. THE has been observed in Cr2Te3 thin films with Bi bilayer nanosheets intercalated. However, the distribution of inserted Bi nanosheets was random, therefore, locating and studying the interface between Bi and Cr2Te3 layers is difficult. The growth scheme of Bi on the Cr2Te3 surface is still blank. In this work, Bi/Cr2Te3 heterostructure thin films were fabricated by molecular beam epitaxy (MBE). The Bi (1 1 0) surface was grown on the Cr2Te3 (0 0 0 1) layer in islands from cross-sectional and plane-view scanning transmission electron microscopy (STEM) observation. THE signals were observed in the Bi/Cr2Te3 heterostructure thin films below 130 K. The two-component anomalous Hall effect (AHE) that might induce similar hump and dip signals near the coercive field was excluded by the minor loop method.en_US
dcterms.accessRightsembargoed accessen_US
dcterms.bibliographicCitationJournal of physical chemistry C, Jan. 9, 2025, v. 129, no. 1, p. 715-721en_US
dcterms.isPartOfJournal of physical chemistry Cen_US
dcterms.issued2025-01-09-
dc.identifier.scopus2-s2.0-85212575738-
dc.identifier.eissn1932-7455en_US
dc.description.validate202506 bchyen_US
dc.description.oaNot applicableen_US
dc.identifier.FolderNumbera3751-
dc.identifier.SubFormID50940-
dc.description.fundingSourceSelf-fundeden_US
dc.description.pubStatusPublisheden_US
dc.date.embargo2025-12-17en_US
dc.description.oaCategoryGreen (AAM)en_US
Appears in Collections:Journal/Magazine Article
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Embargo End Date 2025-12-17
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