The toroidal moment in condensed-matter physics and its relation to the magnetoelectric effect
By N. Spaldin, M. Fiebig, M. Mostovoy. 2008
481 citations recorded by the source corpus.
Subfields: Condensed Matter Physics, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/f7797b845b7082ad109b6a50d5587e4b1eb9e49a
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In Condensed Matter Physics
In Electronic, Optical and Magnetic Materials
Citations in the corpus
- Multiferroic materials and magnetoelectric physics: symmetry, entanglement, excitation, and topology (2015, background): “Besides the ferroelectric order and ferromagnetic order, there exist two more primary ferroic orders [71]: ferroelastic order which breaks neither the time-reversal symmetry nor the space-inversion symmetry [69]; and ferrotoridal order T ∼M × r which breaks both the time-reversal symmetry and the sp”
- Magnetoelectric resonance with electromagnons in a perovskite helimagnet (2011, background): “On the other hand, the magnetoelectric resonance observed at present may be viewed as the dynamical resonance of toroidal momen”
- The evolution of multiferroics (2016, background): “Ferroelectricity originates from two Bi 3+ electrons that shift away from the Bi ion and towards the FeO6 octahedra, giving rise to a spontaneous polarization P along the [111] direction.”
- Ginzburg-Landau theory for skyrmions in inversion-symmetric magnets with competing interactions (2015, unknown): “A measurable quantity associated with the helicity φ0 is the toroidal moment T (φ0) ≡ ∫ dr3r × S ∝ sin φ0 [54].”