Spin Chirality, Berry Phase, and Anomalous Hall Effect in a Frustrated Ferromagnet
By Y. Taguchi, Y. Oohara, Hideki Yoshizawa, N. Nagaosa, Yoshinori Tokura. Science, 2001
603 citations recorded by the source corpus.
Subfields: Condensed Matter Physics, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/21d7cdd9645d3dbc6419d5a120786d38de4fe5d0
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Condensed Matter Physics
- N. Nagaosa
- Y. Tokura
- Patrick Lee
- J. Sinova
- Michel J. P. Gingras
- Allan H. MacDonald
- J. S. Gardner
- J. Greedan
In Electronic, Optical and Magnetic Materials
- N. Nagaosa
- Y. Tokura
- Stuart S. P. Parkin
- Michel J. P. Gingras
- Claudia Felser
- A. Nayak
- J. S. Gardner
- J. Kübler
Citations in the corpus
- Doping a Mott insulator: Physics of high-temperature superconductivity (2004, background): “…chirality will produce the anomalous Hall effect in some ferromagnets such as manganites and pyrochlore oxides, where the non-coplanar spin configurations are realized by thermal excitation of the Skymion or the strong spin anisotropy in the ground state (Ye et al., 1999; Taguchi et al., 2001).”
- Magnetic Pyrochlore Oxides (2009, methodology): “It is well established that the Nd2Mo2O7 phase is a metallic ferromagnet with Tc = 95 K for stoichiometric, polycrystalline samples.”
- Skyrmion lattice with a giant topological Hall effect in a frustrated triangular-lattice magnet (2018, background): “These composite spin parameters couple with charge degrees of freedom in a correlated electron system to show unconventional electromagnetic responses (7-10).”
- Large anomalous Hall effect driven by a nonvanishing Berry curvature in the noncolinear antiferromagnet Mn3Ge (2015, background): “ld parallel to [2-1-10] displays a tiny spontaneous magnetization of 0.005 µ B/Mn at 2 K (Fig. 3). The zero field moment is slightly larger (0.006 µ B/Mn at 2 K) when the field is applied parallel to [01, 2, 3, 4, 5, 6, 7, 8, 9, 10]. An extremely soft magnetic behavior is found in both cases with co”
- Anomalous hall effect (2009, methodology): “Its lattice structure consists of two interpenetrating sublattices comprised of tetrahedrons of Nd and Mo atoms, respectively (the sublattices are shifted along the c-axis) (Taguchi et al., 2001; Yoshii et al., 2000).”