Related Experiment Video
Updated: May 24, 2026

15:58
Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
Published on: December 3, 2013
Spin drift velocity, polarization, and current-driven domain-wall motion in (Ga,Mn)(As,P)
J Curiale1, A Lemaître, C Ulysse
1Laboratoire de Physique des Solides, Université Paris-Sud, CNRS, 91405 Orsay, France.
Physical Review Letters
|March 10, 2012
Summary
Current-driven domain motion in ferromagnetic semiconductors reveals a linear flow regime. Near absolute zero, domain-wall velocity matches spin drift, indicating nonadiabatic spin transfer torque contributions.
Area of Science:
- Spintronics
- Condensed Matter Physics
- Materials Science
Background:
- Ferromagnetic semiconductors are promising for spintronic devices.
- Understanding current-driven domain wall motion is crucial for device applications.
- Perpendicular magnetic anisotropy is key for efficient domain wall manipulation.
Purpose of the Study:
- To investigate current-driven domain-wall motion in (Ga,Mn)(As,P) ferromagnetic semiconductor tracks.
- To explore the relationship between domain-wall velocity and spin drift velocity.
- To analyze the spin transfer torque and current spin polarization.
Main Methods:
- Fabrication of (Ga,Mn)(As,P) ferromagnetic semiconducting tracks.
- Electrical transport measurements to study domain-wall dynamics.
- Temperature-dependent measurements across the ferromagnetic phase.
Main Results:
- A linear steady-state flow regime for domain-wall motion was observed over a wide temperature range (0.1T(c) < T < T(c)).
- Near 0 K, domain-wall velocity equals spin drift velocity, occurring below the intrinsic motion threshold.
- This suggests a nonadiabatic contribution to spin transfer torque.
Conclusions:
- Domain-wall dynamics in (Ga,Mn)(As,P) exhibit a linear flow regime.
- Nonadiabatic spin transfer torque plays a significant role in domain-wall motion at low temperatures.
- The temperature dependence of current spin polarization can be inferred from domain-wall dynamics.
More Related Videos
Related Concept Videos
Drift Velocity
The high speed of electrical signals results from the fact that the force between charges acts rapidly at a distance. Thus, when a free charge is forced into a wire, the incoming charge pushes other charges ahead due to the repulsive force between like charges. These moving charges move the charges farther down the line. The density of charge in a system cannot easily be increased, so the signal is passed on rapidly. The resulting electrical shock wave moves through the system at nearly the...
Potential Due to a Magnetized Object
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
Magnetic Field due to Moving Charges
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...
Atomic Nuclei: Nuclear Relaxation Processes
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis. This...
Atomic Nuclei: Nuclear Spin State Overview
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
The Hall Effect
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.

