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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 ...
A homojunction PN junction.The band at the interface is continuous. In forward bias mode, the depletion width decreases. Both p and n junctions are doped at a 1e15/cm3 doping level, leading to built-in potential of ~0.59 V. Observe the different Quasi Fermi levels for conduction band and valence band in n and p regions (red curves).
Both p and n junctions are doped at a 1e15/cm3 doping level, leading to built-in potential of ~0.59V. Observe the different Quasi Fermi levels for conduction band and valence band in n and p regions (red curves). A depletion region forms instantaneously across a p–n junction.
p–n junction operation in forward bias mode showing reducing depletion width. Both p and n junctions are doped at a 10 15 /cm 3 doping level, leading to built-in potential of ~ 0.59 V. Observe the different quasi-fermi levels for conduction band and valence band in n and p regions (red curves).
Band diagram of PN junction operation in forward bias mode showing reducing depletion width. Both p and n junctions are doped at a 1×10 15 /cm 3 doping level, leading to built-in potential of ~0.59 V. Reducing depletion width can be inferred from the shrinking charge profile, as fewer dopants are exposed with increasing forward bias.
As recombination proceeds and more ions are created, an increasing electric field develops through the depletion zone that acts to slow and then finally stop recombination. At this point, there is a "built-in" potential across the depletion zone. A p–n junction diode in low forward bias mode.
As an example the band bending induced by the forming of a p-n junction or a metal-semiconductor junction can be modified by applying a bias voltage . This voltage adds to the built-in potential ( V B I {\displaystyle V_{BI}} ) that exists in the depletion region ( V B I − V A {\displaystyle V_{BI}-V_{A}} ). [ 6 ]
An application of the flat band potential can be found in the determining the width of the space charge region in a semiconductor-electrolyte junction. [2] Furthermore, it is used in the Mott-Schottky equation to determine the capacitance of the semiconductor-electrolyte junction [ 3 ] [ 4 ] [ 5 ] and plays a role in the photocurrent of a ...