Related Experiment Video
Updated: Jan 19, 2026
01:08
Spin–Spin Coupling Constant: Overview
1.5K
Eigen damping constant of spin waves in ferromagnetic nanostructure
Indra Purnama1, Jung-Hwan Moon2,3, Chun-Yeol You4,5
1Department of Emerging Materials Science, DGIST, Daegu, 42988, South Korea.
Scientific Reports
|September 15, 2019
Summary
Researchers developed a method to reduce spin wave (SW) attenuation by controlling wave shape, not just material properties. This finding could enable more efficient SW-based information carriers and impact wave attenuation control across various fields.
Area of Science:
- Physics
- Materials Science
- Information Technology
Background:
- All waves, including spin waves (SWs), exhibit superposition and attenuation.
- Spin waves are a promising candidate for next-generation information carriers, analogous to photons in photonics.
- High attenuation due to material damping is a major obstacle for practical SW devices.
Purpose of the Study:
- To develop a method for identifying SW eigenmodes.
- To investigate the possibility of reducing SW attenuation.
- To demonstrate that wave attenuation can be controlled by wave shape rather than solely material properties.
Main Methods:
- Developed a novel method to calculate SW eigenmodes.
- Analyzed the eigen damping constants associated with these modes.
- Compared calculated eigen damping constants to typical material damping constants.
Main Results:
- Identified SW eigenmodes with significantly reduced damping.
- Demonstrated that eigen damping constants can be up to 40% lower than bulk material damping.
- Showcased that wave attenuation is controllable via wave shape.
Conclusions:
- Wave attenuation is not exclusively limited by material parameters.
- Controlling the shape of spin waves offers a new pathway to minimize attenuation.
- This breakthrough has implications for advancing SW devices and general wave-based technologies.
Related Concept Videos
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
Ferromagnetism
3.0K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
3.0K
Magnetic Damping
1.0K
Eddy currents can produce significant drag on motion, called magnetic damping. For instance, when a metallic pendulum bob swings between the poles of a strong magnet, significant drag acts on the bob as it enters and leaves the field, quickly damping the motion.
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
1.0K
Damped Oscillations
6.8K
In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Although friction and other non-conservative...
6.8K
Types of Damping
7.6K
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
7.6K
06:43Writing and Low-Temperature Characterization of Oxide Nanostructures
10.4K
Oxide nanostructures provide new opportunities for science and technology. The interfacial conductivity between LaAlO3 and SrTiO3 can be controlled with near-atomic precision using a conductive atomic force microscopy technique. The protocol for creating and measuring conductive nanostructures at LaAlO3/SrTiO3 interfaces is...
10.4K
