Large topological Hall effect in a chiral antiferromagnet in hopping transport regime

The combination of structural chirality and magnetism leads to the formation of spin chirality through noncoplanar magnetic structures, resulting in unusual electronic transport properties. The spin chirality generates nonzero Berry curvature in real space, acting as an emergent magnetic field and contributing to the unconventional anomalous Hall effect, known as the geometrical or topological Hall effect (THE). This study unveils the remarkable occurrence of THE in a chiral antiferromagnetic (AFM) semiconductor <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mi>Eu</a:mi><a:msub><a:mi>Ir</a:mi><a:mn>2</a:mn></a:msub><a:msub><a:mi mathvariant="normal">P</a:mi><a:mn>2</a:mn></a:msub></a:mrow></a:math> in the hopping regime. It exhibits a complex incommensurately spiral AFM ground state due to its chiral crystalline structure, providing fertile ground for the emergence of topologically nontrivial spin textures such as skyrmions. A substantial THE is observed under finite magnetic fields, making <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mi>Eu</c:mi><c:msub><c:mi>Ir</c:mi><c:mn>2</c:mn></c:msub><c:msub><c:mi mathvariant="normal">P</c:mi><c:mn>2</c:mn></c:msub></c:mrow></c:math> an exceptional case within the ultralow-conductivity hopping regime for investigating the interplay between topologically nontrivial magnetic structures and hopping carriers. Owing to its semiconducting nature, we have formulated a theoretical model based on Mott's variable range-hopping mechanism, effectively elucidating the temperature and magnetic field-dependent behavior of THE. <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mrow><e:mi>Eu</e:mi><e:msub><e:mi>Ir</e:mi><e:mn>2</e:mn></e:msub><e:msub><e:mi mathvariant="normal">P</e:mi><e:mn>2</e:mn></e:msub></e:mrow></e:math> thus serves as an ideal candidate for comprehending transport properties in the hopping regime and offers a unique opportunity for the implementation of AFM semiconductor-based spintronic devices. Published by the American Physical Society 2024

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Journal
Physical Review Research
Published
2024-12-19
DOI
https://doi.org/10.1103/physrevresearch.6.043295
Citations
1
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
Field-Weighted Citation Impact
0.31

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article

Large topological Hall effect in a chiral antiferromagnet in hopping transport regime

Maia G. Vergniory, Changjiang Yi, Subhajit Roychowdhury, Yixi Su et al.
1 citations
Physical Review Research
Physics of Superconductivity and Magnetism
0.31
article

Large topological Hall effect in a chiral antiferromagnet in hopping transport regime

Maia G. Vergniory, Changjiang Yi, Subhajit Roychowdhury, Yixi Su, Yishui Zhou, Nikolai Peshcherenko, Premakumar Yanda, Kartik Samanta, Claudia Felser, Yang Zhang, Chandra Shekhar, Qun Yang, Horst Borrmann
article en
1 citations

Abstract

The combination of structural chirality and magnetism leads to the formation of spin chirality through noncoplanar magnetic structures, resulting in unusual electronic transport properties. The spin chirality generates nonzero Berry curvature in real space, acting as an emergent magnetic field and contributing to the unconventional anomalous Hall effect, known as the geometrical or topological Hall effect (THE). This study unveils the remarkable occurrence of THE in a chiral antiferromagnetic (AFM) semiconductor <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mi>Eu</a:mi><a:msub><a:mi>Ir</a:mi><a:mn>2</a:mn></a:msub><a:msub><a:mi mathvariant="normal">P</a:mi><a:mn>2</a:mn></a:msub></a:mrow></a:math> in the hopping regime. It exhibits a complex incommensurately spiral AFM ground state due to its chiral crystalline structure, providing fertile ground for the emergence of topologically nontrivial spin textures such as skyrmions. A substantial THE is observed under finite magnetic fields, making <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mi>Eu</c:mi><c:msub><c:mi>Ir</c:mi><c:mn>2</c:mn></c:msub><c:msub><c:mi mathvariant="normal">P</c:mi><c:mn>2</c:mn></c:msub></c:mrow></c:math> an exceptional case within the ultralow-conductivity hopping regime for investigating the interplay between topologically nontrivial magnetic structures and hopping carriers. Owing to its semiconducting nature, we have formulated a theoretical model based on Mott's variable range-hopping mechanism, effectively elucidating the temperature and magnetic field-dependent behavior of THE. <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mrow><e:mi>Eu</e:mi><e:msub><e:mi>Ir</e:mi><e:mn>2</e:mn></e:msub><e:msub><e:mi mathvariant="normal">P</e:mi><e:mn>2</e:mn></e:msub></e:mrow></e:math> thus serves as an ideal candidate for comprehending transport properties in the hopping regime and offers a unique opportunity for the implementation of AFM semiconductor-based spintronic devices. Published by the American Physical Society 2024

Physical Review ResearchVol. 6(4)
University of California, Los Angeles (US), Forschungszentrum Jülich (DE), Indian Institute of Science Education and Research, Bhopal (IN), Heinz Maier-Leibnitz Zentrum (DE), Max Planck Institute for Chemical Physics of Solids (DE), Donostia International Physics Center (ES), University of Tennessee at Knoxville (US)
Alexander von Humboldt-Stiftung, University of Tennessee, Deutsche Forschungsgemeinschaft, H2020 European Research Council
Openalex Percentile: Top 40%
Physics of Superconductivity and Magnetism
0.31
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