Diode and doping on N and P regions

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    Diode Doping
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SUMMARY

The discussion centers on the characteristics of N and P regions in semiconductor diodes. The N region, rich in electrons, has a number density of electrons that is approximately equal to the number density of donor atoms, while the P region is rich in holes. The doping level, which can reach around 1019 cm-3 for optimal conductivity, plays a crucial role in determining the number of carriers. Even in equilibrium, both regions contain minority carriers, with holes present in the N region due to thermal generation and recombination processes.

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  • Familiarity with carrier concentration equations
  • Basic principles of diode operation
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Electrical engineers, semiconductor physicists, and students studying diode operation and semiconductor materials will benefit from this discussion.

fisico30
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Dear forum,

in a diode semiconductor, the N region is rich in electrons. The P region is rich in holes.

Is the number of extra electrons in the N region equal, larger or smaller than the number of holes in the P region? If so, why?


Also, in the N region, it is said that the majority carriers are the electrons. I get that. The minority carriers are the holes...but there are no holes in the N region so how can there be any minority carriers at all?


Thanks,
fisico30
 
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The number of electrons/holes is a function of doping and can be controlled by the device designer. The doping saturates at around 10^19 cc-1, which is called "extrinsic" doping. It gives the highest conductivity possible which is useful near the electrode connections.

You can inject holes into the n region, where they live for a time (the mean recombination time) before meeting electrons and annihilating. Transistor action is caused by minority carriers injected across the base region into the collector.
 
No, at non-zero temperature, even in equilibrium there are both electrons and holes present in both the n and p region. They fulfill a equilibrium constant equation ##n_en_h=K(T)##. On the n side ##n_e=n_{0e}-n_h\approx n_{0e}## and thus ##n_h\approx K/n_{0e}## where ##n_e## is the number density of electrons ##n_h## the number density of holes and ##n_{0e}## the number density of donor atoms.
A similar equation holds for the p side.
 

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