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Content
           1.Introduction
           2.Semiconductors
           3.Energy band in solids
           4. Conduction band, Valance band and Forbidden gap
           5.Insulators, Conductors and Semiconductors
           6.Electrons and holes in semi conductors
           7.Intrinsic semiconductor
           8.Doping of a semiconductor
           9.Extrinsic semi conductors
           10.N-type semi conductor
           11.P-Type semiconductor

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In the year 1947,              INTRODUCTION
Transistor was
invented by three
scientists.
William Shockley, John
Bardeen and Walter
Brattain in 1956 ,
shared Nobel Prize in
physics for creating the
transistor.
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SEMICONDUCTORS
   Semiconductors have resistivity
   between good conductors and
   insulators.

   The resistivity of semiconductor
   lies approximately in between 10 -2
   ohm m and 10 4 ohm m at room
   temperature.
   .
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ENERGY BANDS IN SOLIDS
           There are discrete energy levels in the
           case of an isolated atom.




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Arrangement of electrons in an isolated Silicon
                         atom




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In solids , the atoms are arranged in a
           systematic space lattice and each atom is
           influenced by neighbouring atoms.
           The closeness of atoms results in the
           intermixing of electrons of neighbourring
           atoms.




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Insulators
             Conduction Band          In an insulator, the forbidden
                                      gap is very large and in
                                      general is more than 3eV.
             FORBIDDEN GAP
                                      No electron is available for
                                      conduction.
Energy




              Valence Band            Large amount of energy is
                                      needed to move electron
                                      from valance band to
               Filled Band            conduction band.

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In the case of semiconductors the
         Semiconductors              forbidden gap is very small.

                                     At 0K the conduction band is
                                     empty and the valence band is
             Conduction Band
                                     completely filled.
             FORBIDDEN GAP
             Around 0.7eV (Ge) and   When a small amount of energy is
             1.1 eV (Si)             supplied, the electrons can easily
                                     jump the forbidden gap.
Energy




              Valence Band
                                     The conductivity of a
                                     semiconductor is of the order of
                                     10 2mho m-1
               Filled Band
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Conductors
                                In conductors there is no forbidden
                                gap.

                                The valence band and the
                                conduction band overlap.

             Conduction Band    The electrons from valence band
                                freely enter into the conduction
                                band due to overlapping of bands.
Energy




             No forbidden gap

                                Therefore very low potential
              Valence Band      difference can cause continuous
                                flow of current.

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Electrons and holes in semiconductors

                             At absolute 0 temperature,
                At 0 K
                             in a pure semiconductor
                             the valence band is
           Conduction Band   completely filled and the
Energy




                             conduction band is vacant.


           Valence Band                Electron




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Electrons and holes in semiconductors

              At Room         At room temperature
              temperature
                              some of the electrons get
            Conduction Band
                              energy to break the
                              covalent bond and moves
  Energy




                              in to the conduction band.


           Valence Band            Electron


                                   Hole



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FORMATION OF N - TYPE MATERIAL




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Group 3 atoms have one less electron
     than silicon so when they are introduced
     into the crystal, there is a ‘hole' where
     one extra electron should be.

      Electrons from neighbouring atoms can
     move into this hole, leaving a hole where
     they used to be which is in turn filled by
     another neighbouring electron.

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FORMATION OF P - TYPE MATERIAL




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BAND THEORY OF SOLIDS

  • 1.
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  • 2.
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  • 3.
    Content 1.Introduction 2.Semiconductors 3.Energy band in solids 4. Conduction band, Valance band and Forbidden gap 5.Insulators, Conductors and Semiconductors 6.Electrons and holes in semi conductors 7.Intrinsic semiconductor 8.Doping of a semiconductor 9.Extrinsic semi conductors 10.N-type semi conductor 11.P-Type semiconductor 9/2/2012 weyes57 3
  • 4.
    In the year1947, INTRODUCTION Transistor was invented by three scientists. William Shockley, John Bardeen and Walter Brattain in 1956 , shared Nobel Prize in physics for creating the transistor. 9/2/2012 weyes57 4
  • 5.
    SEMICONDUCTORS Semiconductors have resistivity between good conductors and insulators. The resistivity of semiconductor lies approximately in between 10 -2 ohm m and 10 4 ohm m at room temperature. . 9/2/2012 weyes57 5
  • 6.
    ENERGY BANDS INSOLIDS There are discrete energy levels in the case of an isolated atom. 9/2/2012 weyes57 6
  • 7.
    Arrangement of electronsin an isolated Silicon atom 9/2/2012 weyes57 7
  • 8.
    In solids ,the atoms are arranged in a systematic space lattice and each atom is influenced by neighbouring atoms. The closeness of atoms results in the intermixing of electrons of neighbourring atoms. 9/2/2012 weyes57 8
  • 9.
    Insulators Conduction Band In an insulator, the forbidden gap is very large and in general is more than 3eV. FORBIDDEN GAP No electron is available for conduction. Energy Valence Band Large amount of energy is needed to move electron from valance band to Filled Band conduction band. 9/2/2012 weyes57 9
  • 10.
    In the caseof semiconductors the Semiconductors forbidden gap is very small. At 0K the conduction band is empty and the valence band is Conduction Band completely filled. FORBIDDEN GAP Around 0.7eV (Ge) and When a small amount of energy is 1.1 eV (Si) supplied, the electrons can easily jump the forbidden gap. Energy Valence Band The conductivity of a semiconductor is of the order of 10 2mho m-1 Filled Band 9/2/2012 weyes57 10
  • 11.
    Conductors In conductors there is no forbidden gap. The valence band and the conduction band overlap. Conduction Band The electrons from valence band freely enter into the conduction band due to overlapping of bands. Energy No forbidden gap Therefore very low potential Valence Band difference can cause continuous flow of current. 9/2/2012 weyes57 11
  • 12.
    Electrons and holesin semiconductors At absolute 0 temperature, At 0 K in a pure semiconductor the valence band is Conduction Band completely filled and the Energy conduction band is vacant. Valence Band Electron 9/2/2012 weyes57 12
  • 13.
    Electrons and holesin semiconductors At Room At room temperature temperature some of the electrons get Conduction Band energy to break the covalent bond and moves Energy in to the conduction band. Valence Band Electron Hole 9/2/2012 weyes57 13
  • 14.
    FORMATION OF N- TYPE MATERIAL 9/2/2012 weyes57 14
  • 15.
    Group 3 atomshave one less electron than silicon so when they are introduced into the crystal, there is a ‘hole' where one extra electron should be. Electrons from neighbouring atoms can move into this hole, leaving a hole where they used to be which is in turn filled by another neighbouring electron. 9/2/2012 weyes57 15
  • 16.
    FORMATION OF P- TYPE MATERIAL 9/2/2012 weyes57 16
  • 17.
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  • 18.
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