topological hall effect
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2022 ◽  
pp. 117619
Author(s):  
Yangkun He ◽  
Sebastian Schneider ◽  
Toni Helm ◽  
Jacob Gayles ◽  
Daniel Wolf ◽  
...  

2021 ◽  
Vol 5 (12) ◽  
Author(s):  
Rabindra Pahari ◽  
Balamurugan Balasubramanian ◽  
Ahsan Ullah ◽  
Priyanka Manchanda ◽  
Hiroaki Komuro ◽  
...  

2021 ◽  
Vol 104 (23) ◽  
Author(s):  
N. Swain ◽  
M. Shahzad ◽  
G. V. Paradezhenko ◽  
A. A. Pervishko ◽  
D. Yudin ◽  
...  

2021 ◽  
Vol 13 (1) ◽  
Author(s):  
Won-Young Choi ◽  
Woosuk Yoo ◽  
Myung-Hwa Jung

AbstractTopological spin textures such as magnetic skyrmions have attracted considerable interest due to their potential application in spintronic devices. However, there still remain several challenges to overcome before their practical application, for instance, achieving high scalability and thermal stability. Recent experiments have proposed a new class of skyrmion materials in the Heusler family, Mn1.4Pt0.9Pd0.1Sn and Mn2Rh0.95Ir0.05Sn, which possess noncollinear magnetic structures. Motivated by these experimental results, we suggest another Heusler compound hosted by Mn3Ga to overcome the above limitations. We fabricate Mn3-xPdxGa thin films, focusing on the magnetic compensation point. In Mn2.3Pd0.7Ga, we find a spin-reorientation transition around TSR = 320 K. Below the TSR, we observe the topological Hall effect and a positive magnetic entropy change, which are the hallmarks of a chiral noncollinear spin texture. By integrating all the data, we determine the magnetic phase diagram, displaying a wide chiral noncollinear spin phase even at room temperature. We believe that this compensated ferrimagnet shows promise for opening a new avenue toward chiral spin-based, high-density, and low-power devices.


Author(s):  
Junshu Chen ◽  
Liang Zhou ◽  
Linjing Wang ◽  
Zijun Yan ◽  
Xintan Deng ◽  
...  

2021 ◽  
Vol 104 (17) ◽  
Author(s):  
Akira Matsui ◽  
Takuya Nomoto ◽  
Ryotaro Arita

2021 ◽  
Vol 104 (17) ◽  
Author(s):  
Md Rafique Un Nabi ◽  
Aaron Wegner ◽  
Fei Wang ◽  
Yanglin Zhu ◽  
Yingdong Guan ◽  
...  

2021 ◽  
Vol 2 (1) ◽  
Author(s):  
Kohei Fujiwara ◽  
Yasuyuki Kato ◽  
Takeshi Seki ◽  
Kentaro Nomura ◽  
Koki Takanashi ◽  
...  

AbstractNon-coplanar spin textures with finite scalar spin chirality can be artificially induced at surfaces and interfaces through the interfacial Dzyaloshinskii-Moriya interaction. However, stabilizing a proper magnetic skyrmion crystal via this route remains elusive. Here, using an epitaxial bilayer of platinum and geometrically frustrated kagome-lattice ferromagnet Fe3Sn, we show the possible formation of a two-dimensional skyrmion crystal under well-regulated Fe3Sn thickness conditions. Magnetization measurements reveal that the magnetic anisotropy is systematically varied from an inherent in-plane type to a perpendicular type with the thickness reduction. Below approximately 0.5 nm, we clearly detect a topological Hall effect that provides evidence for finite scalar spin chirality. Our topological Hall effect analysis, combined with theoretical simulations, not only establishes its interfacial Dzyaloshinskii-Moriya interaction origin, but also indicates the emergence of a stable skyrmion crystal phase, demonstrating the potential of kagome-lattice ferromagnets in spin chirality engineering using thin-film nanostructures.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
F. Tejo ◽  
R. Hernández Heredero ◽  
O. Chubykalo-Fesenko ◽  
K. Y. Guslienko

AbstractA hedgehog or Bloch point is a point-like 3D magnetization configuration in a ferromagnet. Regardless of widely spread treatment of a Bloch point as a topological defect, its 3D topological charge has never been calculated. Here, applying the concepts of the emergent magnetic field and Dirac string, we calculate the 3D topological charge (Hopf index) of a Bloch point and show that due to the magnetostatic energy contribution it has a finite, non-integer value. Thus, Bloch points form a new class of hopfions—3D topological magnetization configurations. The calculated Bloch point non-zero gyrovector leads to important dynamical consequences such as the appearance of topological Hall effect.


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