PN Junction. Silicon vs Germanium

In summary, when connecting P and N materials, the movement of electrons from N to P creates negative and positive ions, resulting in an electric field or barrier potential. However, the number of electrons which recombine does not solely determine the barrier potential, as it also depends on factors such as dielectric constant and effective mass of charge carriers. This is evident in the comparison between P and N doped silicon and germanium, where the barrier potential for germanium is higher despite it having more valence electrons.
  • #1
Goodver
102
1
When we connect P and N materials, electrons from N drift to P, thus create negative ions in P and positive ions in N.

=> electric field (barrier potential) must depend on an amount of electrons recombined with holes in P region.

=> The more electrons recombined, the more ions created, the more barrier potential.

BUT! Silicon has 14 electrons and 4 on the 3d shell. Germanium has 32 electrons and 4 on the 4th shell.

=> at 25C degrees, electrons in N region in Germanium must have more energy than electrons in Silicon, because less energy required to remove electron from an atom => more electrons can drift to P region, thus barrier potential for Germanium should be higher, however

Vbp Germanium = 0.3 V Vbp Silicon = 0.7 V

why?

P.S. I am talking about P doped and N doped silicon compared to the junction between P doped and N doped germanium
 
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  • #2
The number of electrons which recombine does not depend on the number of valence electrons. The potential difference rather depends on things like the dielectric constant of the semiconductors and the effective mass of the charge carriers.
 
  • #3
Thanks DrDu!
 

What is a PN Junction?

A PN Junction is a boundary between a P-type semiconductor and an N-type semiconductor in a diode. It is formed by bringing together a P-type and N-type material, creating a depletion region where electrons and holes combine and form a barrier to current flow.

How does a PN Junction work?

When a PN Junction is formed, the P-type material becomes positively charged due to the loss of electrons, while the N-type material becomes negatively charged due to the excess of electrons. This creates an electric field at the junction, which prevents the flow of current in the reverse direction. In the forward direction, when a voltage is applied, the electric field decreases, allowing current to flow through the diode.

What is the difference between silicon and germanium PN Junctions?

The main difference between silicon and germanium PN Junctions is their bandgap energy. Silicon has a larger bandgap energy compared to germanium, which means it requires more energy to move electrons from the valence band to the conduction band. This makes silicon PN Junctions more efficient at higher temperatures and in high-power applications. Germanium PN Junctions, on the other hand, are more efficient at lower temperatures and in low-power applications.

What are the advantages of using silicon PN Junctions?

Silicon PN Junctions have several advantages over germanium PN Junctions. They have a higher breakdown voltage, meaning they can withstand higher voltages without breaking down. They also have a lower leakage current, which improves their efficiency. Additionally, silicon is more abundant and cheaper to produce compared to germanium.

Can a PN Junction be used for anything other than diodes?

Yes, PN Junctions have a wide range of applications beyond diodes. They are commonly used in transistors, solar cells, and integrated circuits. In transistors, PN Junctions are used to control the flow of current, while in solar cells, they convert light energy into electrical energy. In integrated circuits, PN Junctions act as switches to control the flow of current and perform logical operations.

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