In an intrinsic semiconductors at room temperature current conduction is very less. To increase the conductivity of the semiconductor some suitable impurity (or) doping agent is added.
EXTRINSIC
SEMICONDUCTORS
In
an intrinsic semiconductors at room temperature current conduction is very
less. To increase the conductivity of the semiconductor some suitable impurity
(or) doping agent is added. The process of adding impurities to a semiconductor
is called as doping. This impure form of semiconductor is called as extrinsic
semiconductor. Generally for 106 to 1010 atom of
semiconductor material one impurity atom is added.
The
purpose of adding impurity is to increase either the number of free electrons
(or) holes in a semiconductor. Generally, two types of impurity atoms are added
to the semiconductor namely the impurity atoms containing 5 valence electron
(Pentavalent) and the impurity atoms containing 3 valence electron (Trivalent).
Depending upon the type of impurity atoms added to the semiconductor, the resulting
semiconductor may be of the following two types.
(i)
N-type semiconductors
(ii)
P-type semiconductors
The
semiconductors, which are obtained by introducing pentavalent impurity atoms
are known as N-type semiconductors. The pentavalent impurity is an element from
group V of the periodic table. The elements in this group contain 5 valence
electrons. The typical examples of such elements are phosphorus (P), antimony
(Sb), Arsenic (As) and bismuth (Bi). These elements donate excess electron
carriers.
It
has been observed that when a pentavalent impurity is added to a pure
semiconductor, it displaces some of its atoms. Fig 3.14 shows the structure of
silicon crystal lattice containing as antimony atom at the central position.
It
may be noted that out of 5 valence electrons, 4 electrons will form covalent
bonds by sharing one electron each will the electrons of the neighbouring
atoms. The 5th electron is an extra electron, and is loosely bound
with the antimony atom. This extra electron, if detached from the antimony
atom, will be available as a carrier of the current. The energy required to
detach this electron is of the order of 0.05 ev for silicon and 0.01 ev for
germanium.
After
donation, the impurity atom becomes a positively charged ion and is known as a
donor ion. N-type semiconductor, the current flows due to the movement of
electrons and holes. But a major part of the current flows due to the movement
of electrons. Therefore the electrons in an N-type semiconductor are known as
majority carriers and holes as minority carriers.
The
semiconductors, which are obtained by adding a trivalent impurity atoms are
known as P-type semiconductors. The trivalent impurity is an element group of
III of the periodic table. The elements in this group contain 3 valence
electrons. Examples of such elements are Gallium (Ga), Indium (In), Aluminium
(Al), Boron (B) etc. These elements make available positive charge carriers
because they create holes, which can accept electrons. Therefore, such elements
are known as acceptor (or) P-type impurities.
It
has been observed that when trivalent impurity is added to a pure
semiconductor, it displaces some of its atoms fig.3.16 shows the structure of a
silicon crystal containing an indium atom at the central position. The 3
valence electrons, of an indium atom, forms 3 covalent bonds by sharing one
electron with the electrons of neighbouring atoms. However, the fourth covalent
bond is incomplete. A vacancy, which exists in the incomplete covalent bond
constitutes a hole.
Now,
the indium atom seeks its surrounding atoms so as to acquire the 4th electron,
to complete the covalent bond. It does so by taking an advantage of thermal
motion, which brings one electron form the surrounding atom.
Thus,
an electron, which is in a favourable position is captured by an indium atom.
After doing this, the indium atom becomes an immobile ion. The energy, involved
in capturing the electron to 0.05 ev for silicon and 0.01 ev for germanium.
The
greater number of holes in the valence band than that of electrons in the
conduction band, the Fermi level shifting downwards towards the top of the
valence band as shown in fig.3.17 The addition of a trivalent impurity atom
takes (or) accepts its fourth electrons. After accepting, the impurity atom
becomes a negatively charged ion and is known as an acceptor ion. The P-type
semiconductor the current flows due to the movement of holes and electrons. But
a major part of the current flows due to the movement of holes. Therefore,
holes in a P-type semiconductor are known as majority carriers and electrons as
minority carriers.
Basic Electrical and Electronics Engineering: Unit III: Analog Electronics : Tag: : Energy band diagram, Structural diagram, Properties, Examples - Extrinsic Semiconductors
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