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Connectors p-n is a fundamental semiconductor structure, formed at the interface between two areas of the same semiconductor material with opposite types of conductivity: p-type (dominated by holes as majority carriers) and n-type (where majority carriers are electrons). This creates a potential barrier and a depleted layer, that is the area without free carriers, which acts as a barrier and determines the directionality of current conduction.
In thermodynamic equilibrium, with no external voltage applied, in the p-n junction an internal potential is established due to diffusion of carriers: electrons from the n region move to the p region, and holes vice versa, leading to recombination and the formation of an area without free charges. This region - called the barrier layer - contains the exposed dopant ions, forming an embedded electric field, which counteracts the further flow of carriers.
When the p connector is polarised-n junction in the conduction direction (positive potential to the p part), the potential barrier is lowered, allowing current to flow. When polarised in the negative direction, the barrier increases, and the current is limited to small leakage values. These properties make, that the p-n junction acts as a one-way valve and is the basis for the operation of many semiconductor components, such as rectifier diodes, lEDs, photodiodes, bipolar transistors (BJT) and Unipolar transistors (MOSFET), as well as radiation detectors or light sensors.
Connector parameters p-n - including barrier layer width, potential barrier height and current-voltage characteristics - depend-characteristics - depend on type and level of doping, temperature and geometry of the system. Understanding the behaviour of the p-n junction is crucial for the analysis and design of electronic circuits for both low- and high-power signals, and high power signals.
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