Dember effect

From Wikipedia, the free encyclopedia
Jump to: navigation, search

In physics, the Dember effect is when the electron current from a cathode (I_3) subjected to both illumination and a simultaneous electron bombardment is greater than the sum of the photoelectric current (I_1) and the secondary emission current (I_2).

Discovered by Harry L. Dember (1882–1943) in 1925, this effect is due to the sum of the excitations of an electron by two means: photonic illumination and electron bombardment (i.e. the sum of the two excitations extracts the electron). In Dember’s initial study, he referred only to metals; however, more complex materials have been analyzed since then.

The photoelectric effect due to the illumination of the metallic surface extracts electrons (if the energy of the photon is greater than the extraction work) and excites the electrons which the photons don’t have the energy to extract.

In a similar process, the electron bombardment of the metal both extracts and excites electrons inside the metal.

  I_3-I_2-I_1=I_4 \,

If one considers I_1 a constant and increases I_2, it can be observed that I_4 has a maximum of about 150 times I_1.

On the other hand, considering I_2 a constant and increasing the intensity of the illumination I_2 the I_4, supplementary current, tends to saturate. This is due to the usage in the photoelectric effect of all the electrons excited (sufficiently) by the primary electrons of I_1.

The Dember effect has no relation to the financial market's "December effect". See January effect.

See also[edit]

References[edit]

External links[edit]