Semiconductors Material:
Normally forth group elements in periodic table are semiconductors.
For Example Si, Ge, etc
(Silicon – 14 – 2,8,4) (Germanium – 32 – 2,8,18,4)
Electronic configuration shows that they have four electrons in outer most orbits. We know that atoms in a molecule becomes stable with 8 electronics in outermost orbit. So 4 electrons in outermost orbit of Si or Ge, which is half the maximum possibility in outermost orbit, becomes an important factor which make semiconductors very useful.
Semiconductors Materials other than Forth Group Elements:
Semiconductor material can also be designed using combination of third and fifth group elements.
For example:
GaAs, Ga AlP, GaAlAsP, etc
These semiconductor material more useful because here we get some more forms of semiconductor material like:
Direct type semiconductors
Indirect type semiconductors
Degenerate semiconductors.
(We will discuss these topics later.)
Concept of Electron hole pair in Semiconductors:
At room temperature some electrons are ready to conduct in an electronic circuit. As they will get energy, they will move. So in an unbiased semiconductor material electrons are bounded but they are free to move so they are called free electrons.
When an electron leaves its place, a negative charge leaves the place, so a compensatory positive charge at this place becomes present which is due to absence of a charged particle. This charged particle is called ‘Hole’.
Now it is also easy to understand that a hole is always ready to be generated when a free electron is ready to be generated. So electron hole are generated in pair.
Conductivity in Si and Ge elements:
As we know that the forth group element Si and Ge are having 4 electrons in their outer most orbit. Therefore they are tightly packed structures. Hence their electron affinity is very large means they require a large amount of energy to make an electron free or to break covalent chemical bonding. It emphasize that conduction in Si and Ge is very low. It is obvious that at room temperature, very few electrons and holes are free. So conductivity of pure semiconductor is very low.
Remember: Pure Semiconductor is known as Intrinsic semiconductor.
Impurity Atoms and Doping Process:
Now we have understood that conductivity of pure semiconductor is very low. To increase conductivity of semiconductor, we require to increasing the number of free charge carriers.
To increase free charge carriers, we require adding some extra atoms in the pure semiconductor material. These atoms are known as Impurity atoms.
The process of adding impurity atoms in the semiconductor material, is known as Doping Process.
There are two types of Doping processes
Acceptor impurity atom: III A group elements of periodic table have only 3 valence electrons (Trivalent atoms) and therefore when these atoms are added to the Si or Ge atoms, an electron vacant place is created which behaves as a free hole. Examples are Al, Ga, etc (Element from III A group).
Donor impurity atom: V A group elements of periodic table have 5 valence electrons (pentavalent atoms) and therefore when these atoms are added to the Si or Ge atoms, an extra electron is attached to the element which behaves as a free electron. Examples are Al, Ga, etc (Element from V A group) .
Types of Semiconductor Materials:
There are two types of Semiconductor materials
(No of electrons = No of Holes)
(No of electrons ≠ No of Holes)
So we have two cases (Two Types of Extrinsic Material):
(Negative charges > positive charges) (n type material)
(Negative charges < positive charges) (p type material)
Majority and Minority Charge Carrier:
We know that there are two types of charge carriers in a semiconductor material.
The charge carrier which is larger in concentration is known as majority charge carrier.
The charge carrier which is smaller in concentration is known as minority charge carrier.
Since number of electrons is equal to number of holes in intrinsic semiconductors therefore there is no any majority or minority concept.
In Extrinsic semiconductor, number of electron electrons and number of holes are unequal. So we can say one carrier is majority and another is minority.
Semiconductor Type (n,p) Majority Minority
N Type n > p electrons holes
P Type n < p holes electrons





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