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P–n junction
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P–n junction
A p–n junction is a combination of two types of semiconductor materials, p-type and n-type, in a single crystal. The "n" (negative) side contains freely-moving electrons, while the "p" (positive) side contains freely-moving electron holes. Connecting the two materials causes creation of a depletion region near the boundary, as the free electrons fill the available holes, which in turn allows electric current to pass through the junction only in one direction.
p–n junctions represent the simplest case of a semiconductor electronic device; a p-n junction by itself, when connected on both sides to a circuit, is a diode. More complex circuit components can be created by further combinations of p-type and n-type semiconductors; for example, the bipolar junction transistor (BJT) is a semiconductor in the form n–p–n or p–n–p. Combinations of such semiconductor devices on a single chip allow for the creation of integrated circuits.
Solar cells and light-emitting diodes (LEDs) are essentially p-n junctions where the semiconductor materials are chosen, and the component's geometry designed, to maximise the desired effect (light absorption or emission). A Schottky junction is a similar case to a p–n junction, where instead of an n-type semiconductor, a metal directly serves the role of the "negative" charge provider.
The invention of the p–n junction is usually attributed to American physicist Russell Ohl of Bell Laboratories in 1939. Two years later (1941), Vadim Lashkaryov reported discovery of p–n junctions in Cu2O and silver sulphide photocells and selenium rectifiers. The modern theory of p-n junctions was elucidated by William Shockley in his classic work Electrons and Holes in Semiconductors (1950).
A p-doped semiconductor (that is, one where impurities such as Boron are introduced into its crystal lattice) is relatively conductive. The same is true of an n-doped semiconductor, but the junction between them - the boundary where the p-doped and n-doped semiconductor materials meet - can become depleted of charge carriers such as electrons, depending on the relative voltages of the two semiconductor regions.
By manipulating the flow of charge carriers across this depleted layer, p–n junctions can be used as diodes: circuit elements that allow a flow of electricity in one direction but not in the opposite direction. This property makes the p–n junction extremely useful in modern semiconductor electronics.
Bias is the application of a voltage relative to a p–n junction region:
Negative charge carriers (electrons) can easily flow through the junction from n to p but not from p to n, and the reverse is true for positive charge carriers (Electron hole). When the p–n junction is forward-biased, charge carriers flow freely due to the reduction in energy barriers seen by electrons and holes. When the p–n junction is reverse-biased, however, the junction barrier (and therefore resistance) becomes greater and charge flow is minimal.
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P–n junction
A p–n junction is a combination of two types of semiconductor materials, p-type and n-type, in a single crystal. The "n" (negative) side contains freely-moving electrons, while the "p" (positive) side contains freely-moving electron holes. Connecting the two materials causes creation of a depletion region near the boundary, as the free electrons fill the available holes, which in turn allows electric current to pass through the junction only in one direction.
p–n junctions represent the simplest case of a semiconductor electronic device; a p-n junction by itself, when connected on both sides to a circuit, is a diode. More complex circuit components can be created by further combinations of p-type and n-type semiconductors; for example, the bipolar junction transistor (BJT) is a semiconductor in the form n–p–n or p–n–p. Combinations of such semiconductor devices on a single chip allow for the creation of integrated circuits.
Solar cells and light-emitting diodes (LEDs) are essentially p-n junctions where the semiconductor materials are chosen, and the component's geometry designed, to maximise the desired effect (light absorption or emission). A Schottky junction is a similar case to a p–n junction, where instead of an n-type semiconductor, a metal directly serves the role of the "negative" charge provider.
The invention of the p–n junction is usually attributed to American physicist Russell Ohl of Bell Laboratories in 1939. Two years later (1941), Vadim Lashkaryov reported discovery of p–n junctions in Cu2O and silver sulphide photocells and selenium rectifiers. The modern theory of p-n junctions was elucidated by William Shockley in his classic work Electrons and Holes in Semiconductors (1950).
A p-doped semiconductor (that is, one where impurities such as Boron are introduced into its crystal lattice) is relatively conductive. The same is true of an n-doped semiconductor, but the junction between them - the boundary where the p-doped and n-doped semiconductor materials meet - can become depleted of charge carriers such as electrons, depending on the relative voltages of the two semiconductor regions.
By manipulating the flow of charge carriers across this depleted layer, p–n junctions can be used as diodes: circuit elements that allow a flow of electricity in one direction but not in the opposite direction. This property makes the p–n junction extremely useful in modern semiconductor electronics.
Bias is the application of a voltage relative to a p–n junction region:
Negative charge carriers (electrons) can easily flow through the junction from n to p but not from p to n, and the reverse is true for positive charge carriers (Electron hole). When the p–n junction is forward-biased, charge carriers flow freely due to the reduction in energy barriers seen by electrons and holes. When the p–n junction is reverse-biased, however, the junction barrier (and therefore resistance) becomes greater and charge flow is minimal.
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