Related Experiment Video
Updated: Mar 15, 2026

09:06
Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
8.7K
Magnetic Yoking and Tunable Interactions in FePt-Based Hard/Soft Bilayers.
Dustin A Gilbert1,2, Jung-Wei Liao3, Brian J Kirby2
1Dept. of Physics, University of California, Davis, California 95616, USA.
Scientific Reports
|September 9, 2016
Summary
Researchers discovered a magnetic yoking effect in FePt hard/soft bilayers. The soft layer
Area of Science:
- Nanomagnetism and Spintronics
- Materials Science
Background:
- Magnetic interactions are fundamental to nanomagnetic and spintronic devices.
- Understanding and controlling these interactions is key for advanced applications.
Purpose of the Study:
- To demonstrate and characterize a magnetic yoking effect in FePt-based hard/soft bilayers.
- To show how soft layer thickness tunes magnetic interactions from exchange-dominated to dipolar-dominated.
Main Methods:
- Experimental techniques including first-order reversal curves (FORC) and polarized neutron reflectometry (PNR).
- The ΔM method for analyzing magnetic hysteresis.
- Micromagnetic simulations for theoretical confirmation.
Main Results:
- A sensitive magnetic yoking effect was observed, mediated by the soft layer.
- The soft layer's thickness dictates the interaction type: thin layers promote exchange coupling, while thicker layers induce dipolar coupling.
- Tunable magnetic interactions were achieved by controlling the soft layer thickness.
Conclusions:
- The magnetic yoking effect provides an effective strategy for designing and controlling magnetic interactions.
- This approach is applicable to a wide range of magnetic nanostructures and devices.
- Findings pave the way for novel nanomagnetic and spintronic device architectures.
More Related Videos
Related Concept Videos
Ferromagnetism
3.4K
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...
3.4K
Magnetic Force Between Two Parallel Currents
4.8K
Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
4.8K
Magnetic Susceptibility and Permeability
2.6K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
2.6K
Magnetic Damping
1.2K
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...
1.2K
Paramagnetism
3.1K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
3.1K
Magnetostatic Boundary Conditions
1.7K
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
1.7K

