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Extrinsic Semiconductors
Rida Batool
Extrinsic Semiconductors
• Semiconductive materials do not conduct current well and are of limited value in
their intrinsic state
• This is because of the limited number of free electrons in the conduction band and
holes in the valence band.
• Intrinsic silicon (or germanium) must be modified by increasing the number of free
electrons or holes to increase its conductivity and make it useful in electronic
devices.
• An extrinsic semiconductor is a semiconductor doped by a specific impurity
which is able to deeply modify its electrical properties, making it suitable for
electronic applications.
Doping
• Since semiconductors are generally poor conductors, their conductivity can be
drastically increased by the controlled addition of impurities to pure semiconductive
material.
• The process of adding impurities is called doping which increases the number of
current carriers (electrons or holes).
• Based on the impurities present in the Extrinsic Semiconductors, they are classified
into two categories.
• N-type Semiconductors
• P-type Semiconductors
N-Type Semiconductors
• To increase the number of conduction-band electrons in intrinsic silicon,
pentavalent impurity atoms are added.
• These are atoms with five valence electrons such as arsenic (As), phosphorus
(P), bismuth (Bi), and antimony (Sb).
• In the given figure, each pentavalent atom (antimony, in this case) forms
covalent bonds with four adjacent silicon atoms.
• Four of the antimony atom’s valence electrons are used to form the covalent
bonds with silicon atoms, leaving one extra electron.
N-Type Semiconductors
• The fifth electron is weakly bound to the parent atom. And even for lesser
thermal energy it is released Leaving the parent atom positively ionized.
• This extra electron becomes a conduction electron because it is not involved
in bonding. Because the pentavalent atom gives up an electron, it is often
called a donor atom.
• A conduction electron created by this doping process does not leave a hole
in the valence band because it is in excess of the number required to fill the
valence band.
Majority and Minority Carriers
• Since most of the current carriers are electrons, silicon (or germanium) doped with
pentavalent atoms is an n-type semiconductor (the n stands for the negative charge
on an electron).
• The electrons are called the majority carriers in n-type material.
• Although the majority of current carriers in n-type material are electrons, there are
also a few holes that are created when electron-hole pairs are thermally generated.
• These holes are not produced by the addition of the pentavalent impurity atoms.
Holes in an n-type material are called minority carriers.
2nd leacture

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2nd leacture

  • 2. Extrinsic Semiconductors • Semiconductive materials do not conduct current well and are of limited value in their intrinsic state • This is because of the limited number of free electrons in the conduction band and holes in the valence band. • Intrinsic silicon (or germanium) must be modified by increasing the number of free electrons or holes to increase its conductivity and make it useful in electronic devices. • An extrinsic semiconductor is a semiconductor doped by a specific impurity which is able to deeply modify its electrical properties, making it suitable for electronic applications.
  • 3. Doping • Since semiconductors are generally poor conductors, their conductivity can be drastically increased by the controlled addition of impurities to pure semiconductive material. • The process of adding impurities is called doping which increases the number of current carriers (electrons or holes). • Based on the impurities present in the Extrinsic Semiconductors, they are classified into two categories. • N-type Semiconductors • P-type Semiconductors
  • 4. N-Type Semiconductors • To increase the number of conduction-band electrons in intrinsic silicon, pentavalent impurity atoms are added. • These are atoms with five valence electrons such as arsenic (As), phosphorus (P), bismuth (Bi), and antimony (Sb). • In the given figure, each pentavalent atom (antimony, in this case) forms covalent bonds with four adjacent silicon atoms. • Four of the antimony atom’s valence electrons are used to form the covalent bonds with silicon atoms, leaving one extra electron.
  • 5.
  • 6. N-Type Semiconductors • The fifth electron is weakly bound to the parent atom. And even for lesser thermal energy it is released Leaving the parent atom positively ionized. • This extra electron becomes a conduction electron because it is not involved in bonding. Because the pentavalent atom gives up an electron, it is often called a donor atom. • A conduction electron created by this doping process does not leave a hole in the valence band because it is in excess of the number required to fill the valence band.
  • 7. Majority and Minority Carriers • Since most of the current carriers are electrons, silicon (or germanium) doped with pentavalent atoms is an n-type semiconductor (the n stands for the negative charge on an electron). • The electrons are called the majority carriers in n-type material. • Although the majority of current carriers in n-type material are electrons, there are also a few holes that are created when electron-hole pairs are thermally generated. • These holes are not produced by the addition of the pentavalent impurity atoms. Holes in an n-type material are called minority carriers.