Faraday effect

The Faraday effect has a few applications in measuring instruments.

Around the band gap, the Faraday effect shows resonance behavior.

This difference in phase velocities leads to the Faraday effect.

It is a magneto-optical phenomenon with a similar origin to the Faraday effect.

This Faraday effect is one of the first discoveries of the relationship between light and electromagnetic effects.

This is now termed the Faraday effect.

These effects are in addition to what is known as the Faraday effect, a polarization of light caused by intergalactic magnetic fields.

Radio waves passing through the Earth's ionosphere are likewise subject to the Faraday effect.

Cotton then became interested in the Faraday effect near absorption lines and demonstrated magnetic circular dichroism.

In the Faraday effect, the polarization of light can be rotated when passed through a transparent medium to which an external magnetic field is applied.

This rotation occurs near its atomic absorption lines by the Faraday effect and anomalous dispersion.

This component then produces an ac variation in the plane of polarization via the longitudinal Faraday effect.

The combination of the two is described by gyroelectromagnetic media, for which gyroelectricity and gyromagnetism (Faraday effect) may occur at the same time.

For instance, the Faraday effect has been used to measure optical rotatory power and for remote sensing of magnetic fields.

The Faraday effect is used in spintronics research to study the polarization of electron spins in semiconductors.

It is similar to the Faraday effect where the plane of polarization of the transmitted light is rotated.

Thermal neutrons can be polarized by transmission through magnetic materials in a method analogous to the Faraday effect for photons.

The Verdet constant is an optical "constant" that describes the strength of the Faraday effect for a particular material.

The Faraday effect, discovered by Michael Faraday in 1845, was the first experimental evidence that light and electromagnetism are related.

The Faraday effect is caused by left and right circularly polarized waves propagating at slightly different speeds, a property known as circular birefringence.

The magnetic field, ', applied to the Faraday rotator causes a rotation in the polarization of the light due to the Faraday effect.

The inverse Faraday effect is the effect opposite to the Faraday effect.

The Faraday effect is chromatic (i.e. it depends on wavelength) and therefore the Verdet constant is quite a strong function of wavelength.

The Faraday effect will rotate the plane of polarization of a beam passing through a plasma with a magnetic field in the direction of the beam.

Depending on the component of the magnetization along the z-direction, Mz, the optical beam experiences a rotation of its polarization due to the Faraday effect.