pn junction

PN Junction Theory

In the previous tutorial we saw how to make an N-type semiconductor material by doping a silicon atom with small amounts of Antimony and also how to make a P-type semiconductor material by doping another silicon atom with Boron.

This is all well and good, but these newly doped N-type and P-type semiconductor materials do very little on their own as they are electrically neutral. However, if we join (or fuse) these two semiconductor materials together they behave in a very different way merging together and producing what is generally known as a “PN Junction“.

When the N-type semiconductor and P-type semiconductor materials are first joined together a very large density gradient exists between both sides of the PN junction. The result is that some of the free electrons from the donor impurity atoms begin to migrate across this newly formed junction to fill up the holes in the P-type material producing negative ions.

However, because the electrons have moved across the PN junction from the N-type silicon to the P-type silicon, they leave behind positively charged donor ions ( ND ) on the negative side and now the holes from the acceptor impurity migrate across the junction in the opposite direction into the region where there are large numbers of free electrons.

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As a result, the charge density of the P-type along the junction is filled with negatively charged acceptor ions ( NA ), and the charge density of the N-type along the junction becomes positive. This charge transfer of electrons and holes across the PN junction is known as diffusion. The width of these P and N layers depends on how heavily each side is doped with acceptor density NA, and donor density ND, respectively.

This process continues back and forth until the number of electrons which have crossed the junction
have a large enough electrical charge to repel or prevent any more charge carriers from crossing over the junction. Eventually a state of equilibrium (electrically neutral situation) will occur producing a “potential barrier” zone around the area of the junction as the donor atoms repel the holes and the acceptor atoms repel the electrons.

Since no free charge carriers can rest in a position where there is a potential barrier, the regions on either sides of the junction now become completely depleted of any more free carriers in comparison to the N and P type materials further away from the junction. This area around the PN Junction is now called the Depletion Layer.

The PN junction

semiconductor pn junction

The total charge on each side of a PN Junction must be equal and opposite to maintain a neutral charge condition around the junction. If the depletion layer region has a distance D, it therefore must therefore penetrate into the silicon by a distance of Dp for the positive side, and a distance of Dn for the negative side giving a relationship between the two of  Dp.NA = Dn.ND  in order to maintain charge neutrality also called equilibrium.

PN Junction Distance

semiconductor pn junction distance

As the N-type material has lost electrons and the P-type has lost holes, the N-type material has become positive with respect to the P-type. Then the presence of impurity ions on both sides of the junction cause an electric field to be established across this region with the N-side at a positive voltage relative to the P-side. The problem now is that a free charge requires some extra energy to overcome the barrier that now exists for it to be able to cross the depletion region junction.

This electric field created by the diffusion process has created a “built-in potential difference” across the junction with an open-circuit (zero bias) potential of:

PN junction potential

Where: Eo is the zero bias junction voltage, VT the thermal voltage of 26mV at room temperature, ND and NA are the impurity concentrations and ni is the intrinsic concentration.

A suitable positive voltage (forward bias) applied between the two ends of the PN junction can supply the free electrons and holes with the extra energy. The external voltage required to overcome this potential barrier that now exists is very much dependent upon the type of semiconductor material used and its actual temperature.

Typically at room temperature the voltage across the depletion layer for silicon is about 0.6 – 0.7 volts and for germanium is about 0.3 – 0.35 volts. This potential barrier will always exist even if the device is not connected to any external power source, as seen in diodes.

The significance of this built-in potential across the junction, is that it opposes both the flow of holes and electrons across the junction and is why it is called the potential barrier. In practice, a PN junction is formed within a single crystal of material rather than just simply joining or fusing together two separate pieces.

The result of this process is that the PN junction has rectifying current–voltage (IV or I–V) characteristics. Electrical contacts are fused onto either side of the semiconductor to enable an electrical connection to be made to an external circuit. The resulting electronic device that has been made is commonly called a PN junction Diode or simply Signal Diode.

Then we have seen here that a PN junction can be made by joining or diffusing together differently doped semiconductor materials to produce an electronic device called a diode which can be used as the basic semiconductor structure of rectifiers, all types of transistors, LED’s, solar cells, and many more such solid state devices.

In the next tutorial about the PN junction, we will look at one of the most interesting applications of the PN junction is its use in circuits as a diode. By adding connections to each end of the P-type and the N-type materials we can produce a two terminal device called a PN Junction Diode which can be biased by an external voltage to either block or allow the flow of current through it.


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  • D
    Dean Boi

    this site is very helpful.

  • b
    bhavesh singh


  • B
    Bhuvaneshwar Singh Yadav

    Good explanation.what about drift of charges

  • K
    Khaled Mohammed

    Can I get more information about Diodes and Thyristors?

  • C

    Thank you

  • L
    Lameck Ngulinga

    Excellent explanation. But need more on drift and diffusion current .

  • k
    kawembe paul Ngesa

    Nice explanation no complain here

  • N

    A p-n junction diode in thermal equilibrium, is forward biased. then suddenly the supply is cut off. it doesnt have anymore force to push the charges cross the barrier. I have a doubt here. Literally the diode must return to thermal equilibrium i.e. back with barrier potential (depletion region). Since the last moment the electrons have recombined with the holes in the p -side creating -ve charged atoms over entire p side (like all holes recombined with electrons) But how it regains its state of equilibrium back. what happens immediately when supply is cut off. could you explain plz… sry if at any part it sounded dumb.

  • D

    I have a doubt which is similar to Gaurav’s,

    1. When both N & P are equally doped then it will have equal number of electrons and holes. Therefore there should not be any extra ions present in depletion layer.
    2. When N-type is doped higher than P-type, then only -ve will be there in depletion layer and vice-versa

    My doubt is, why both holes and electrons available in depletion layer at the same time when there are more opposites charges are there to fill?
    Please correct if mistaken any thing here.

    • D
      Devangana Roy

      it is known that depletion layer penetrates more into lightly doped region.
      Wp:width of depletion layer lying in p-side
      Wn:width of depletion layer in n-side
      Na:concentration of acceptor ions in p- side
      Nd:concentration of donor ions on n -side
      So according to this relationship if doping concentration is high then depletion width portion in that region would be less and vice-versa.Also if p side and n side have same doping concentration then portion of depletion width would be same in both regions.

  • f

    Thanks for the Tutorials on this Website,,I couldn’t Go without saying that I have been empowered by the wide scope of Resources

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