Related Experiment Video
Updated: Aug 6, 2026

12:22
Optimization, Test and Diagnostics of Miniaturized Hall Thrusters
Published on: February 16, 2019
Coherence control of Hall charge and spin currents
Hui Zhao1, Eric J Loren, H M van Driel
1Laboratory for Photonics & Quantum Electronics, 138 IATL, University of Iowa, Iowa City, Iowa 52242, USA.
Physical Review Letters
|August 16, 2006
Summary
Researchers generated pure spin and charge currents in gallium arsenide (GaAs) using optical pulses. Varying laser properties controlled current type and direction without external fields.
Area of Science:
- Spintronics
- Optoelectronics
- Solid-state physics
Background:
- Generating and controlling pure spin and charge currents is crucial for next-generation electronic devices.
- Optical techniques offer a promising, field-free method for manipulating charge and spin dynamics in semiconductors.
Purpose of the Study:
- To investigate the generation of pure spin and charge currents in intrinsic gallium arsenide (GaAs) using two-color optical coherence control.
- To demonstrate the ability to tune the type, magnitude, and direction of these currents by manipulating optical parameters.
Main Methods:
- Utilized two-color optical coherence control with orthogonally and parallel polarized femtosecond pulses (70 fs) at 1430 nm and 715 nm.
- Performed experiments at cryogenic temperatures (80 K) in intrinsic GaAs.
- Varied the relative phase and polarization of the incident laser pulses.
Main Results:
- Generated a pure spin source current yielding a transverse Hall pure charge current with orthogonally polarized pulses.
- Generated a pure charge source current yielding a pure spin current with parallel polarized pulses.
- Demonstrated effective tuning of both source and transverse currents' type, magnitude, and direction by adjusting optical parameters.
Conclusions:
- Optical coherence control provides a versatile, field-free method for generating and manipulating pure spin and charge currents in GaAs.
- This technique opens possibilities for novel spintronic device functionalities and optical control of charge/spin dynamics.
Related Concept Videos
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.
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...
Magnetic Force Between Two Parallel Currents
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...
Force On A Current Loop In A Magnetic Field
Magnetic forces on wires carrying current are most frequently applied in motors. A DC motor is a device that converts electrical energy into mechanical work. In motors, wire loops are enclosed in a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate. The direction of the current is reversed once the loop's surface area is lined up with the magnetic field, causing a constant torque on the loop. During the process, commutators...
Torque On A Current Loop In A Magnetic Field
The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
Magnetic Field Of A Current Loop
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.

