When a small amount of pentavalent impurity (group V element) is doped to a pure semiconductor, it becomes n-type semiconductor.
When
a small amount of pentavalent impurity (group V element) is doped to a pure
semiconductor, it becomes n-type semiconductor.
Such
impurities are known as donor impurities because they donate free electrons to
semiconductor crystal.
Typical
examples of pentavalent impurities are phosphorus, (Atomic No. 15) and antimony
(Atomic No. 51).
Covalent bond in n-type
semiconductor
A
pentavalent impurity (phosphorus) having five valence electrons is added to a
pure semiconductor having four valence electrons (silicon or germanium).
Now,
four electrons of germanium form a covalent bond with four valence electrons of
phosphorus (impurity atom).
The
fifth electron which is now free finds no place in covalent bond structure as
shown in fig. 3.7 (a).
We have one electron left free. This acts as a conduction electron. A very small amount of energy (0.01 eV for germanium and 0.05 eV for silicon) is needed to detach this fifth electron.
The
addition of pentavalent impurity gives a large number of free electrons
(negative charges) in semiconductor. Therefore, it is called n-type
semiconductor where n stands for negative type.
Since
every pentavalent atom contributes one free electron, in addition to thermally
generated electron-hole pairs, the number of free electrons is more than the
number of holes in n-type semiconductor.
Thus
in this case, electrons are majority charge carriers and holes are minority
charge carriers.
Energy band of n-type semiconductor
The
energy band diagram of n-type semiconductor is shown in fig.3.7 (b). When the
donor impurities are added, the allowable energy levels (donor energy levels)
are introduced.
These
donor energy levels are slightly below the conduction band. They are discrete
and do not form a band because the impurity atoms are far away in the crystal
and hence their interaction is small.
The
donor energy level for germanium is 0.01 eV and for silicon it is 0.05 eV below
the conduction band. Therefore, even at room temperature, almost all the fifth
electrons enter into the conduction band.
Physics for Electronics Engineering: Unit III: Semiconductors and Transport Physics : Tag: : Covalent bond, Energy band, Crystal Structure, Diagram - n - type Semiconductor
Physics for Electronics Engineering
PH3254 - Physics II - 2nd Semester - ECE Department - 2021 Regulation | 2nd Semester ECE Dept 2021 Regulation