Related Experiment Video
Updated: Feb 3, 2026

08:42
Using Multi-fluorinated Bile Acids and In Vivo Magnetic Resonance Imaging to Measure Bile Acid Transport
Published on: November 27, 2016
11.6K
Single-Shot Multi-Level All-Optical Magnetization Switching Mediated by Spin Transport
Satoshi Iihama1,2, Yong Xu1, Marwan Deb1
1Institut Jean Lamour, UMR CNRS 7198, Université de Lorraine, 54506, Vandoeuvre-lés-Nancy, France.
Advanced Materials (Deerfield Beach, Fla.)
|October 19, 2018
Summary
Ultrafast magnetization switching using single laser pulses was achieved in Co/Pt multilayers. This breakthrough enables deterministic control of magnetic states for advanced data storage.
Area of Science:
- Optics and Magnetism
- Materials Science
- Nanotechnology
Background:
- All-optical ultrafast magnetization switching is key for energy-efficient magnetic storage.
- Current methods often require external magnetic fields or multiple optical pulses.
- GdFeCo ferrimagnetic films are known to switch with a single pulse.
Purpose of the Study:
- To demonstrate single-pulse all-optical magnetization switching in Co/Pt multilayers.
- To explore the potential of Co/Pt multilayers in spin-valve structures for magnetic storage.
- To investigate deterministic switching of ferromagnetic layers using optical pulses.
Main Methods:
- Utilized femtosecond (fs) laser pulses for all-optical switching experiments.
- Investigated a [Co/Pt]/Cu/GdFeCo magnetic spin-valve structure.
- Analyzed spin-polarized currents generated by light-matter interactions.
Main Results:
- Achieved single-pulse magnetization switching in Co/Pt multilayers within a spin-valve.
- Demonstrated access to four distinct magnetic configurations using sequential fs pulses.
- Identified spin-polarized currents from GdFeCo as the determinant of the [Co/Pt] layer's final state.
Conclusions:
- This work presents a novel approach for deterministic all-optical switching of ferromagnetic layers.
- The findings pave the way for engineering materials for opto-magnetic multi-bit recording.
- Enables development of ultrafast and energy-efficient magnetic storage technologies.
Related Concept Videos
Carrier-Mediated Transport
1.3K
Carrier-mediated transport is a pivotal process in drug absorption, particularly for lipid-insoluble drugs, and encompasses facilitated diffusion and active transport. Facilitated diffusion allows drugs to move along their concentration gradient without energy expenditure, while active transport utilizes ATP to drive drug movement against this gradient.
Active transport involves two types of membrane-spanning transporters: uptake and efflux. Uptake transporters are expressed in the small...
Active transport involves two types of membrane-spanning transporters: uptake and efflux. Uptake transporters are expressed in the small...
1.3K
Switching of BJT
861
Switching behavior in Bipolar Junction Transistors (BJTs) is a fundamental aspect utilized in various electronic circuits, particularly for digital logic applications like switches and amplifiers. In a typical switching circuit, a BJT alternates between cut-off and saturation modes, corresponding to the "off" and "on" states, respectively, thus behaving like an ideal switch.
Cut-off Mode ("Off" State): In this state, both the emitter-base and collector-base junctions are...
Cut-off Mode ("Off" State): In this state, both the emitter-base and collector-base junctions are...
861
Colors and Magnetism
14.1K
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...
14.1K
NMR Spectroscopy: Spin–Spin Coupling
3.2K
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...
3.2K
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
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

