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Photocathode

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photocathode [¦fōd·ō′kath‚ōd]
(electronics)
A photosensitive surface that emits electrons when exposed to light or other suitable radiation; used in phototubes, television camera tubes, and other light-sensitive devices.

Photocathode 

a cathode in certain vacuum-tube devices that emits electrons when exposed to light. Photocathodes are usually made of substances based on compounds consisting of elements from groups I and V or groups I and VI of the periodic system of elements.

The most widely used types of photocathodes are cesium oxide-silver, cesium antimonide (Cs3Sb), and trialkali photocathodes. Cesium oxide-silver photocathodes consist of Cs2O containing free cesium and free silver. Trialkali photocathodes are made of Sb-Cs, Sb-K, and Sb-Na compounds. The emissive material is deposited as a monomolecular layer on a metal or glass substrate. A photocathode may be either opaque or semitransparent. An opaque photocathode is exposed to light through the vacuum; a semitransparent photocathode is exposed through the substrate.

The main parameter characterizing the efficiency of a photocathode is the luminous sensitivity, which is equal to the ratio of the photoelectric current and the luminous flux that produces the current. For example, the luminous sensitivity of opaque cesium oxide-silver and cesium antimonide photocathodes is 100–120 microamperes per lumen (µA/lm); the luminous sensitivity of opaque trialkali photocathodes may be as high as 1,000 µA/lm, and that of semitransparent trialkali photocathodes is 600 µA/lm.

A new type of photocathode, called the negative-electron-affinity (NEA) photocathode, was developed in the 1960’s (seeELECTRON AFFINITY). NEA photocathodes include photocathodes made of III-V compounds—for example, GaAs photocathodes, which are sensitive to visible light, and InAsP and InGaAs photocathodes, which are sensitive to visible light and to infrared radiation at wavelengths of up to 1.5 micrometers. The luminous sensitivity of opaque NEA photocathodes may be as high as or even exceed 1,500 µA/lm. The luminous sensitivity of semitransparent NEA photocathodes is relatively low. Thus, the luminous sensitivity of GaAs photocathodes with a film thickness of 1–2 micrometers does not exceed 400(µA/lm; that is, it is lower than the luminous sensitivity of semitransparent trialkali photocathodes.

The production technology for NEA photocathodes is considerably more complex than that for conventional photocathodes. Hence, NEA photocathodes are not widely used.

P. V. TIMOFEEV



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The microchannel plate sits inside a vacuum package between the photocathode and the electron-collecting semiconductor array.
Achieving Counting Statistics in Current Mode Operation In current mode detection, counting statistics appears as the RMS width in the sample distribution, due to the fluctuation in the number of electrons produced at the photocathode of the VPD, as a result of the quasi instantaneous amount of energy deposited in the CsI crystal.
The light particles, called photons, are converted into electrons as soon as they hit a photocathode tube; their numbers are multiplied and then sent to hit the back of a fluorescent screen where they regenerate the image.
 
 
 
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