carrier density

A system thus cools slower, the higher the carrier density is.

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

The carrier density was varied by means of the persistent photoconductivity effect.

Thus, the temperature is increased for the gain spectra at higher carrier densities.

As a result, the Hall effect is very useful as a means to measure either the carrier density or the magnetic field.

Experimentally tested the intrinsic minority carrier density for silicon (J10).

It is common to all systems that the laser is an inverted carrier density system.

Results show that the electron–electron scattering rate increases linearly as a function of the carrier densities.

Normally, this "carrier density" increases gradually as a function of doping.

In a normal metal wire, the resistivity also increases as the carrier density decreases.

A laser is, thus, always a high carrier density system that entails many-body interactions.

Charge carrier density denotes the number of charge carriers per volume.

The equilibrium carrier density that results from the balance of these interactions is predicted by thermodynamics.

However, the resistance continues to decrease as the charge carrier density in the conduction band increases.

The scattering rate is calculated using the Fermi golden rule, as a function of the carrier densities.

However in our work, both the peak gain and its position in wavelength are made functions of the carrier density.

The carrier density is obtained by integrating the charge density over the energy that the charges are allowed to have.

A reduced carrier density means that the electronic energy band of the majority carriers is bent away from the Fermi level.

Thus, the larger the carrier density, heat capacity and speed, and the less significant the scattering, the higher is the conductivity.

The kinetic inductance increases as the carrier density decreases.

The term "hot" refers to the effective temperature used to model carrier density, not to the overall temperature of the device.

The dependence of carrier lifetime on the carrier density is expressed as:

However, most of the interesting behavior is seen at low carrier densities, where the system is insulating, or not too far from the metal-insulator transition.

The carrier density (mostly minority carriers) is small and only a very small reverse saturation current flows.

So the carrier density eventually falls back to below lasing threshold which results in the termination of the optical output.