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Colossal magnetoresistance in the multiple wave vector charge density wave regime of an antiferromagnetic Dirac semimetal

Colossal negative magnetoresistance is a well-known phenomenon, notably observed in hole-doped ferromagnetic manganites. It remains a major research topic due to its potential in technological applications. In contrast, topological semimetals show large but positive magnetoresistance, originated fro...

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Detalles Bibliográficos
Autores principales: Singha, Ratnadwip, Dalgaard, Kirstine J., Marchenko, Dmitry, Krivenkov, Maxim, Rienks, Emile D. L., Jovanovic, Milena, Teicher, Samuel M. L., Hu, Jiayi, Salters, Tyger H., Lin, Jingjing, Varykhalov, Andrei, Ong, N. Phuan, Schoop, Leslie M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Association for the Advancement of Science 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10575584/
https://www.ncbi.nlm.nih.gov/pubmed/37831777
http://dx.doi.org/10.1126/sciadv.adh0145
Descripción
Sumario:Colossal negative magnetoresistance is a well-known phenomenon, notably observed in hole-doped ferromagnetic manganites. It remains a major research topic due to its potential in technological applications. In contrast, topological semimetals show large but positive magnetoresistance, originated from the high-mobility charge carriers. Here, we show that in the highly electron-doped region, the Dirac semimetal CeSbTe demonstrates similar properties as the manganites. CeSb(0.11)Te(1.90) hosts multiple charge density wave modulation vectors and has a complex magnetic phase diagram. We confirm that this compound is an antiferromagnetic Dirac semimetal. Despite having a metallic Fermi surface, the electronic transport properties are semiconductor-like and deviate from known theoretical models. An external magnetic field induces a semiconductor metal–like transition, which results in a colossal negative magnetoresistance. Moreover, signatures of the coupling between the charge density wave and a spin modulation are observed in resistivity. This spin modulation also produces a giant anomalous Hall response.