electron-hole pair

These electron-hole pairs can only move along the surface.

Then the collision create a cold carrier and an additional electron-hole pair.

An electron-hole pair is often referred to as an exciton.

First by making use of high energy photons producing two electron-hole pairs.

This generates an electron-hole pair and sometimes heat depending on the band structure.

But we are not to take a mutual potential of electron-hole pair into the Hamiltonian.

This is often described as a charge separated electron-hole pair when working with semiconductors.

This process is known as electron-hole pair generation.

As the light source is scanned across the surface of the silicon, electron-hole pairs are generated.

The absorption of light, generating either electron-hole pairs or excitons.

But only those electron-hole pairs generated in and near the depletion region contribute to current generation.

Then, the field in the avalanche region reaches its maximum value and the population of the electron-hole pairs starts building up.

Larger dots have more closely spaced energy levels in which the electron-hole pair can be trapped.

Incoming infrared radiation is absorbed in the material by the creation of an electron-hole pair.

The absorbed light causes generation of electron-hole pairs.

As described above, when a photon is absorbed by a solar cell it can produce an electron-hole pair.

Absorption of a photon creates an electron-hole pair, which could potentially contribute to the current.

This increases the volume where electron-hole pairs can be generated by an incident photon.

This wider depletion width enables electron-hole pair generation deep within the device.

Electron-hole pairs can be created when suitable electromagnetic radiation falls upon a semiconductor.

It can be said that photons absorbed in the semiconductor create mobile electron-hole pairs.

The number of electron-hole pairs in the steady state at a given temperature is determined by quantum statistical mechanics.

As ionizing radiation passes through the semiconductor, many electron-hole pairs are produced along the track.

The number of electron-hole pairs is proportional to the energy of the radiation to the semiconductor.

When a photon of sufficient energy strikes the diode, it creates an electron-hole pair.