Related Experiment Video
Updated: Jan 6, 2026

06:53
Scanning SQUID Study of Vortex Manipulation by Local Contact
Published on: February 1, 2017
7.2K
Nonlocal Spin Transport as a Probe of Viscous Magnon Fluids
Camilo Ulloa1, A Tomadin2, J Shan3
1Institute for Theoretical Physics, Utrecht University, Princetonplein 5, 3584 CC Utrecht, Netherlands.
Physical Review Letters
|October 2, 2019
Summary
Magnons exhibit fluid-like behavior in ferromagnets. Viscosity in this magnon fluid regime causes a detectable sign change in nonlocal resistance, revealing new insights into spin transport dynamics.
Area of Science:
- Condensed Matter Physics
- Spintronics
- Magnonics
Background:
- Magnons, the quanta of magnetic excitations in ferromagnets, exhibit complex behaviors.
- Understanding magnon dynamics is crucial for advancing spintronic devices and information processing.
Purpose of the Study:
- To theoretically investigate the hydrodynamic regime of magnons in ferromagnets.
- To explore the influence of viscosity on magnon chemical potential and nonlocal resistance.
- To establish nonlocal magnon spin transport devices as a platform for studying fluid dynamics.
Main Methods:
- Theoretical analysis of magnon behavior in the hydrodynamic regime.
- Application of quasiconservation laws for momentum and spin in a magnon fluid.
- Solving equations for nonlocal spin transport in devices with metallic leads.
Main Results:
- Viscous effects in the hydrodynamic regime lead to a sign change in the magnon chemical potential.
- A corresponding sign change in nonlocal resistance is predicted, observable at specific injector-detector distances.
- Finite viscosity results in a magnon backflow phenomenon near the injector lead.
Conclusions:
- Nonlocal resistance measurements can detect the hydrodynamic behavior of magnons.
- Magnon fluid dynamics offer a new perspective on spin transport phenomena.
- Nonlocal magnon spin transport devices are promising for exploring fluid dynamics in magnetic systems.
More Related Videos
Related Concept Videos
Spin–Spin Coupling Constant: Overview
1.4K
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...
1.4K
Magnetic Vector Potential
1.5K
In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
1.5K
Magnetic Field due to Moving Charges
11.4K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
11.4K
Magnetic Susceptibility and Permeability
2.2K
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...
2.2K
NMR Spectroscopy: Spin–Spin Coupling
2.9K
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...
2.9K
Viscosity of Fluid
1.1K
Viscosity measures the resistance a fluid offers to flow and deformation. It results from internal friction between layers of fluid moving relative to one another. Dynamic viscosity, denoted by the Greek letter mu (μ), quantifies the force needed to move one fluid layer over another. For Newtonian fluids like water and air, the relationship between the shearing stress and the rate of shearing strain is linear, meaning their viscosity remains constant regardless of the applied stress.
1.1K

