charge carrier

This results in only a small number of effective charge carriers.

Magnetic forces give information about the charge carriers in a material through the Hall effect.

I would be surprised if it is true, because there are no particularly god charge carriers in liquid O2.

This effect is proportional to the mass of the charge carriers.

In a vacuum, free electrons can act as charge carriers.

There is only one type of charge carrier present.

Therefore, on average there will be no overall motion of charge carriers in any particular direction over time.

So we can imagine that pure ice having no charge carriers would also be a poor conductor.

As you probably already know, in order for anything to conduct electricity, there must be some mobile charge carrier.

The model can be applied to positive (hole) charge carriers, as demonstrated by the Hall effect.

There are two recognized types of charge carriers in semiconductors.

The influence of free charge carriers is often (but not always) unwanted, and various means have been proposed to remove them.

The Court heard arguments involving how much an airport can charge carriers to land their planes.

The more charge carriers that are available, the more current a material can conduct.

It achieved high speed by reducing the charge carrier's transit time.

With most metals the Hall effect indicates electrons are the charge carriers.

These positive and negative ions represent the charge carriers in solution.

The free electrons are therefore the charge carrier in a typical solid conductor.

Below certain width the charge carriers can tunnel through the depletion region.

This effect occurs most efficiently in regions of low charge carrier density.

Also, surface defects in the crystal structure can act as charge carrier traps.

Charge carriers are separated and physically transported to a position of increased electric potential.

Charge carriers in the materials will diffuse when one end of a conductor is at a different temperature from the other.

The flow of charge carriers between the hot and cold regions in turn creates a voltage difference.

The induced polarization will follow the charge carrier when it is moving through the medium.