Related Experiment Video
Updated: Jan 27, 2026

09:17
Use of an Optical Trap for Study of Host-Pathogen Interactions for Dynamic Live Cell Imaging
Published on: July 28, 2011
13.4K
Optically Driven Collective Spin Excitations and Magnetization Dynamics in the Néel-type Skyrmion Host GaV_{4}S_{8}
P Padmanabhan1, F Sekiguchi1, R B Versteeg1
1Physics Institute II, University of Cologne, 50937 Cologne, Germany.
Physical Review Letters
|April 2, 2019
Summary
Researchers optically induced spin excitations in GaV4S8 multiferroic semiconductor. This discovery offers new methods for controlling magnetic order in skyrmion-hosting materials.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Magnetism
Background:
- Gallium Vanadium Tetrasulfide (GaV4S8) exhibits multiferroic properties.
- It hosts stable cycloid (Cyc) and Néel-type skyrmion lattice (SkL) magnetic phases.
- Understanding spin dynamics in these complex magnetic phases is crucial for novel electronic applications.
Purpose of the Study:
- To investigate the coherent generation of collective spin excitations in the Cyc and SkL phases of GaV4S8.
- To elucidate the underlying mechanisms driving these spin excitations.
- To explore the potential for optical control of magnetic order in skyrmion materials.
Main Methods:
- Time-resolved magneto-optical Kerr spectroscopy was employed to probe spin dynamics.
- Micromagnetic simulations were utilized to model the observed phenomena.
- Optical induction of uniaxial anisotropy modulation was investigated.
Main Results:
- Coherent generation of collective spin excitations was successfully demonstrated in both Cyc and SkL phases.
- Optically induced modulation of uniaxial anisotropy was identified as the driving mechanism.
- The study provides insights into spin dynamics in anisotropic skyrmion systems.
Conclusions:
- The findings illuminate spin dynamics in anisotropic materials featuring skyrmions.
- A novel pathway for the optical manipulation of magnetic order in GaV4S8 is established.
- This research opens avenues for advanced spintronic devices utilizing skyrmion manipulation.
Related Concept Videos
ATP Driven Pumps II: P-type Pumps
6.2K
The P-type pumps are a large family of integral membrane transporter ATPases. They are divided into five major types based on substrate specificity, from I to V.
A typical P-type pump has three cytosolic domains: nucleotide-binding (N), phosphorylation (P), and activator (A) domains. These domains are connected to the membrane-spanning helices by short amino acid segments. ATP hydrolysis and covalent phosphoenzyme intermediate formation are crucial parts of the catalytic cycle. At the highly...
A typical P-type pump has three cytosolic domains: nucleotide-binding (N), phosphorylation (P), and activator (A) domains. These domains are connected to the membrane-spanning helices by short amino acid segments. ATP hydrolysis and covalent phosphoenzyme intermediate formation are crucial parts of the catalytic cycle. At the highly...
6.2K
ATP Driven Pumps III: V-type Pumps
4.7K
V-type pumps are ATP-driven pumps found in the vacuolar membranes of plants, yeast, endosomal and lysosomal membranes of animal cells, plasma membranes of a few specialized eukaryotic cells, and some prokaryotes. They are also known as the V1Vo-ATPase, that couple ATP hydrolysis to transport protons against a concentration gradient.
The peripheral or cytosolic V1 domain with eight subunits is involved in ATP hydrolysis. The integral or transmembrane V0 domain containing at least five subunits...
The peripheral or cytosolic V1 domain with eight subunits is involved in ATP hydrolysis. The integral or transmembrane V0 domain containing at least five subunits...
4.7K
Colors and Magnetism
14.0K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
14.0K
Spin–Spin Coupling Constant: Overview
1.5K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.5K
NMR Spectroscopy: Spin–Spin Coupling
3.0K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
3.0K
Spin–Spin Coupling: One-Bond Coupling
1.5K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.5K

