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The Sigma Insight: Energy Bands in Solids and Semiconductors
The World of Semiconductors Imagine a material that can't decide whether it wants to be a conductor like copper or an insulator like rubber
That's a semiconductor for you! In its pure form, known as an intrinsic semiconductor, it behaves almost like an insulator at absolute zero. But as you turn up the heat, something magical happens. The thermal energy excites electrons, allowing them to break free from their covalent bonds and jump from the valence band to the conduction band. Every time an electron makes this leap, it leaves behind a vacancy called a hole. Both the free electrons and the holes act as charge carriers. So, as temperature increases, the number of charge carriers increases, which means the conductivity shoots up. And what happens to resistance when conductivity goes up? It goes down! So, the resistance of an intrinsic semiconductor decreases with an increase in temperature.
The Art of Doping Now, pure semiconductors are cool, but they aren't very useful because their conductivity is too low
To make them useful, we introduce impurities in a process called doping.
If we take pure Silicon, which has 4 valence electrons, and dope it with a trivalent impurity (like Boron or Aluminum, which have 3 valence electrons), the impurity atom forms covalent bonds with three neighboring Silicon atoms. But it falls short by one electron to bond with the fourth Silicon atom. This missing electron creates a vacancy, or a hole. Since we are creating an abundance of holes (which act as positive charge carriers), this type of material is called a -type semiconductor.
On the flip side, what if we dope Silicon with a pentavalent impurity (like Phosphorus or Arsenic, which have 5 valence electrons)? Four of these electrons will form bonds with neighboring Silicon atoms, but the fifth electron is left loosely bound and becomes a free electron. Because we are introducing an abundance of free electrons (negative charge carriers), this material is called an -type semiconductor.
So, in an -type semiconductor, the majority carriers are electrons, and the minority carriers are holes.
The Magic of the - Junction When you take a piece of -type material and join it seamlessly with an -type material, you create a - junction
At the junction, electrons from the -side diffuse into the -side and recombine with holes, creating a depletion region that acts as a barrier.
If you apply a voltage such that the positive terminal is connected to the -side and the negative to the -side (forward bias), the barrier shrinks, and current flows easily. But if you reverse the connections (reverse bias), the barrier widens, and almost no current flows. This ability to allow current in only one direction is the exact definition of a diode. Therefore, a - junction acts as a semiconductor diode.
The Final Verdict Looking back at our options, statement (c) claims that the majority carriers in -type semiconductors are holes
As we've just discovered, -type materials are teeming with extra electrons donated by pentavalent impurities. Therefore, electrons are the majority carriers, making statement (c) the false statement we were looking for!
Similar Questions
JEE Main 2021
LEVELJEE Main
Statement I: By doping silicon semiconductor with pentavalent material, the electrons density increases. Statement II: The n-type semiconductor has net negative charge. In the light of the above statements, choose the most appropriate answer from the options given below.
(A)
Statement I is true but statement II is false.
(B)
Statement I is false but statement II is true.
(C)
Both statement I and statement II are true.
(D)
Both statement I and statement II are false.
JEE Main 2021
LEVELJEE Main
For extrinsic semiconductors when doping level is increased,
(A)
Fermi level of p-type semiconductor will go upward and Fermi level of n-type semiconductors will go downward
(B)
Fermi level of p-type semiconductors will go downward and Fermi level of n-type semiconductor will go upward
(C)
Fermi level of p and n-type semiconductors will not be affected
(D)
Fermi level of both p-type and n-type semiconductors will go upward for K and downward for K, where is Fermi temperature
JEE Main 2021
LEVELJEE Main
In a semiconductor, the number density of intrinsic charge carriers at is . If the semiconductor is doped with impurity atom, the hole density increases to . The electron density in the doped semiconductor is ...... .
JEE Advanced 1997
LEVELBoard
Holes are charge carriers in
* Multiple Correct Options
(A)
intrinsic semiconductors
(B)
ionic solids
(C)
p-type semiconductors
(D)
metals
LEVELBoard
The impurity atoms with which pure silicon should be doped to make a -type semiconductor are those of
* Multiple Correct Options
(A)
phosphorus
(B)
boron
(C)
antimony
(D)
aluminium
JEE Main 2019
LEVELJEE Main
Mobility of electrons in a semiconductor is defined as the ratio of their drift velocity to the applied electric field. If for an -type semiconductor, the density of electrons is and their mobility is , then the resistivity of the semiconductor (since, it is an -type semiconductor contribution of holes is ignored) is close to
(A)
(B)
(C)
(D)
LEVELJEE Main
When a potential difference is applied across, the current passing through
* Multiple Correct Options
(A)
an insulator at is zero
(B)
a semiconductor at is zero
(C)
a metal at is finite
(D)
a - diode at is finite, if it is reverse biased
LEVELBoard
At absolute zero, Si acts as
(A)
non-metal
(B)
metal
(C)
insulator
(D)
None of the above
LEVELJEE Main
Carbon, silicon and germanium have four valence electrons each. At room temperature, which one of the following statements is most appropriate? [AIEEE 2007]
(A)
The number of free conduction electrons is significant in C but small in Si and Ge
(B)
The number of free conduction electrons is negligibly small in all the three
(C)
The number of free electrons for conduction is significant in all the three
(D)
The number of free electrons for conduction is significant only in Si and Ge but small is C
LEVELJEE Main
The electrical conductivity of a semiconductor increases when electromagnetic radiation of wavelength shorter than , is incident on it. The band gap in (eV) for the semiconductor is
(A)
(B)
(C)
(D)
