Something strange about doping semiconductors

In summary, the conversation discusses the realization of a reversal of electronegativity when dissolving a small amount of Gallium arsenide in Silicon. This results in Gallium acting as a source of holes and Arsenic acting as a source of electrons, with the resulting oxidation states of +III and -III for both elements. This is similar to the reaction of ammonia with hydrogen, where the energy gained in forming additional bonds with the host material overrules the electronegativity differences. It is noted that the high dielectric constant of the host material may also play a role in stabilizing the free electrons.
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DrDu
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TL;DR Summary
Doping leads to a reversal of electronegativity
Some post involving diodes made me reconsider pn junctions, with I first learned almost 40 years ago. Coming from a chemistry background, something always felt strange, but I could not tell what. Now I realized:

While e.g. Gallium arsenide is a semiconductor itself and can be described roughly as an ionic compound made of Ga 3+ and As 3- ions, if we dissolve a small amount of it in Silicium, something strange happens. Gallium acts as a source of holes, while Arsenic acts as a source of electrons. If both dopants are present in the same material, or in close proximity like in a PN junction, the electron and holes recombine and we are formally left with Ga- and As+ ions.

So somehow dissolution of GaAs in Si resulted in a reversal of electronegativity. It would be interesting to see when and how this change of oxidation states occurs as a ratio of mixing of GaAs and Si, assuming that the crystal structure does not change.
 
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In fact, the oxidation states of Ga and As remain +III and -III, respectively, Si has a higher electronegativity than Ga, but a lower one than As. As both Ga and As form 4 polar bonds with Si, the resulting oxidation states are +III and -III. We may compare this to the reaction of ammonia with hydrogen: 2 NH3+H2 -> 2 NH4+ + 2e- (in real life, you need some electron acceptor to stabilize the free electrons. In semiconductors, the high dielectric constant of the host may be sufficient to stabilize the electrons in addition to the entropy gain at low doping levels). So, as in chemistry, the energy gained in forming additional bonds with the host material overrules the electronegativity differences.
 
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1. What is doping in semiconductors?

Doping in semiconductors is the process of intentionally adding impurities to a semiconductor material in order to alter its electrical properties. This is done to create either a p-type or n-type semiconductor, which can be used to control the flow of electrons and create electronic devices.

2. How does doping affect the conductivity of semiconductors?

Doping changes the number of free charge carriers (electrons or holes) in a semiconductor material, which in turn affects its conductivity. In p-type semiconductors, the addition of impurities creates more holes, making it easier for electrons to move through the material. In n-type semiconductors, the added impurities create more electrons, increasing the conductivity of the material.

3. What are some common doping materials used in semiconductors?

Common doping materials for p-type semiconductors include boron, aluminum, and gallium, while common doping materials for n-type semiconductors include phosphorus, arsenic, and antimony. These elements are chosen for their ability to create either a deficit or excess of electrons in a semiconductor material.

4. How does doping affect the band gap of semiconductors?

The addition of impurities through doping can either increase or decrease the band gap of a semiconductor material. In p-type semiconductors, the band gap decreases due to the presence of holes, while in n-type semiconductors, the band gap increases due to the presence of extra electrons. This change in band gap affects the material's ability to conduct electricity.

5. What are some applications of doped semiconductors?

Doped semiconductors are used in a wide range of electronic devices, including transistors, diodes, and solar cells. By controlling the flow of electrons and holes, doped semiconductors allow for the creation of electronic circuits and the conversion of light into electricity. They are also used in the production of computer chips and other microelectronic devices.

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