conduction electron

The Knight shift is due to the conduction electrons in metals.

These conduction electrons are the charge carriers in metal conductors.

Therefore, the conduction electrons never get close enough to the ion cores to feel their full force.

One could picture the conduction electrons flowing around them like a river around an island or a big rock.

In one of these, a tensor interaction between conduction electrons was proposed (Walker).

This means that at 0 kelvin, there are no free conduction electrons, and the resistance is infinite.

Physically, this means that it will depend on how conduction electrons interact with the atoms within a given material.

Here, particles correspond to conduction electrons, and antiparticles to holes.

Although the phenomenological description is incorrect for conduction electrons, it can serve as a preliminary treatment.

In this case the interaction between the f-electrons, which present a local magnetic moment and the conduction electrons is neglected.

They are collective oscillations of the conduction electrons like a ripple in the electronic ocean.

In the same manner, because they are much less massive, thermal energy is readily borne by mobile conduction electrons.

Thus Fermi-Dirac statistics is needed for conduction electrons in a typical metal.

Metals are typically also good conductors of heat, but the conduction electrons only contribute partly to this phenomenon.

The oscillatory nature of the conduction electron polarisation was established in rare earth alloys.

Below , the localized f-electrons hybridize with the conduction electrons.

Johnson, Direct measurement of the conduction electron spin relaxation time in gold, Phys.

Spin lifetimes of conduction electrons in metals are relatively short (typically less than 1 nanosecond).

In a dielectric only one of either the conduction electrons or the dipole relaxation typically dominates loss.

Radiation resistance is caused by the radiation reaction of the conduction electrons in the antenna.

In crystalline materials, the wave vectors of conduction electrons are very close to the Fermi surface.

In most metallic samples the muon's positive charge is collectively screened by a cloud of conduction electrons.

Engel had suggested a correlation between the number of conduction electrons and the crystal structure of the metals.

It includes the energy in all the chemical bonds, and the energy of the free, conduction electrons in metals.

Thus, these materials do not have free conduction electrons, and the bonding electrons reflect only a small fraction of the incident wave.