<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Cho SW</submitter><funding>Korea institute of Science and Technology</funding><funding>National Research Foundation (KR)</funding><funding>Ministry of Land, Infrastructure and Transport</funding><funding>National Research Foundation</funding><pagination>2</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9832196</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>10(1)</volume><pubmed_abstract>The interplay between ferromagnetism and the non-trivial topology has unveiled intriguing phases in the transport of charges and spins. For example, it is consistently observed the so-called topological Hall effect (THE) featuring a hump structure in the curve of the Hall resistance (R&lt;sub>xy&lt;/sub>) vs. a magnetic field (H) of a heterostructure consisting of a ferromagnet (FM) and a topological insulator (TI). The origin of the hump structure is still controversial between the topological Hall effect model and the multi-component anomalous Hall effect (AHE) model. In this work, we have investigated a heterostructure consisting of Bi&lt;sub>x&lt;/sub>Sb&lt;sub>2-x&lt;/sub>Te&lt;sub>y&lt;/sub>Se&lt;sub>3-y&lt;/sub> (BSTS) and Cr&lt;sub>2&lt;/sub>Te&lt;sub>3&lt;/sub> (CT), which are well-known TI and two-dimensional FM, respect</pubmed_abstract><journal>Nano convergence</journal><pubmed_title>Investigation of the mechanism of the anomalous Hall effects in Cr&lt;sub>2&lt;/sub>Te&lt;sub>3&lt;/sub>/(BiSb)&lt;sub>2&lt;/sub>(TeSe)&lt;sub>3&lt;/sub> heterostructure.</pubmed_title><pmcid>PMC9832196</pmcid><funding_grant_id>NRF-2021M3F3A2A01037814</funding_grant_id><funding_grant_id>Innovative Talent Education Program for Smart City</funding_grant_id><funding_grant_id>NRF-2021M3F3A2A01037738</funding_grant_id><funding_grant_id>2E31550</funding_grant_id><funding_grant_id>NRF-2020R1A2C200373211</funding_grant_id><funding_grant_id>NRF-2021M3F3A2A03017782</funding_grant_id><funding_grant_id>NRF-2021R1A2C3011450</funding_grant_id><pubmed_authors>Kim S</pubmed_authors><pubmed_authors>Lee S</pubmed_authors><pubmed_authors>Chang YJ</pubmed_authors><pubmed_authors>Khim YG</pubmed_authors><pubmed_authors>Cho SW</pubmed_authors><pubmed_authors>Lee Y</pubmed_authors><pubmed_authors>Choi J</pubmed_authors><pubmed_authors>Park SY</pubmed_authors><pubmed_authors>Han S</pubmed_authors><pubmed_authors>Jo Y</pubmed_authors><pubmed_authors>Lee IH</pubmed_authors></additional><is_claimable>false</is_claimable><name>Investigation of the mechanism of the anomalous Hall effects in Cr&lt;sub>2&lt;/sub>Te&lt;sub>3&lt;/sub>/(BiSb)&lt;sub>2&lt;/sub>(TeSe)&lt;sub>3&lt;/sub> heterostructure.</name><description>The interplay between ferromagnetism and the non-trivial topology has unveiled intriguing phases in the transport of charges and spins. For example, it is consistently observed the so-called topological Hall effect (THE) featuring a hump structure in the curve of the Hall resistance (R&lt;sub>xy&lt;/sub>) vs. a magnetic field (H) of a heterostructure consisting of a ferromagnet (FM) and a topological insulator (TI). The origin of the hump structure is still controversial between the topological Hall effect model and the multi-component anomalous Hall effect (AHE) model. In this work, we have investigated a heterostructure consisting of Bi&lt;sub>x&lt;/sub>Sb&lt;sub>2-x&lt;/sub>Te&lt;sub>y&lt;/sub>Se&lt;sub>3-y&lt;/sub> (BSTS) and Cr&lt;sub>2&lt;/sub>Te&lt;sub>3&lt;/sub> (CT), which are well-known TI and two-dimensional FM, respect</description><dates><release>2023-01-01T00:00:00Z</release><publication>2023 Jan</publication><modification>2026-05-10T06:41:02.432Z</modification><creation>2024-11-14T12:05:46.717Z</creation></dates><accession>S-EPMC9832196</accession><cross_references><pubmed>36625963</pubmed><doi>10.1186/s40580-022-00348-0</doi></cross_references></HashMap>